main linac quadrupoles
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Main Linac Quadrupoles. Th. Zickler CERN. Outlook. Introduction Drive Beam Quadrupoles (DBQ) Requirements and constraints The ‘two-current’ proposal Proposed quadrupole layout Magnetic field calculations and characteristics Main Beam Quadrupoles (MBQ) Requirements and constraints - PowerPoint PPT PresentationTRANSCRIPT
CLI
C W
orks
hop
07
16th
-18
th O
ctob
er 2
007
Tho
mas
Zic
kler
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T/M
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MI/
tz
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Main Linac Quadrupoles
Th. Zickler
CERN
CLI
C W
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hop
07
16th
-18
th O
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er 2
007
Tho
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Zic
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MI/
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2
Outlook
Introduction Drive Beam Quadrupoles (DBQ)
– Requirements and constraints
– The ‘two-current’ proposal
– Proposed quadrupole layout
– Magnetic field calculations and characteristics
Main Beam Quadrupoles (MBQ)– Requirements and constraints
– Proposed quadrupole layout
– Magnetic field calculations and characteristics
– Open issues
Conclusions and future work
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16th
-18
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007
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Introduction
Drive Beam
– 24 Drive Beam Decelerating Sectors (DES) per CLIC Linac
– 856 quadrupoles (428 focusing and 428 defocusing) per DES
– Linear beam energy decrease from 2.38 GeV to 0.24 GeV
– 41 100 quadrupoles needed per Linac
Main Beam
– 2001 Main Beam quadrupoles per CLIC Linac
– Beam energy increase requires variation of integrated gradient in the range between 15 Tm/m and 370 Tm/m
– Baseline: 4 magnet types of different length
– Alternative: several magnets of one type connected in series
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Drive Beam Quadrupoles DBQ
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DBQ Requirements and Constraints
Aperture and field requirements
– Nominal beam energy: 2.5 GeV
– Integrated gradient / beam energy: 5.7 T/GeV
– Integrated gradient: 14.3 Tm/m
– Aperture radius: 13 mm
– Total length (incl. BPM): < 344 mm
Keep heat dissipation into tunnel as low as possible
– Indirect water cooling
No redundancy possible
– High reliability and very robust design (low MTBF)
Large number of magnets (> 40 000!)
– Automated production (50/day in 3 years)
– To be respected already in the preliminary design
– Cost optimization (also for cables and power converters)
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‘Two-Current’ Proposal
‘Two-current’ proposal by H. Braun:
– Splitting the coils in two sub-coils (red & blue)
– Connect all sub-coils of the same type in series (string)
– Power the strings with different current (Ired & Iblue)
– Linear gradient decrease along the string
first quadrupole
mid sector quadrupole
last quadrupole
second quadrupole
second to last quadrupole
Picture by courtesy of H. Braun
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‘Two-Current’ Proposal
Advantages:
– Reduced number of power converters (minimum 4)
– Reduced cable length
Disadvantages:
– Number of turns must be multiple integer of number of magnets per string
– Large number of coil types issue for mass production
– High voltage drop
– Longitudinal beam dynamics in case of PETS failure
– Non-linearity of magnetic field along the string due to iron saturation
Open questions:
– Coupled circuits (power converter design)
Optimum number of magnets per string has to be found
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Proposed DBQ Layout
Assumption: 16 quadrupoles per string
2.5 GeV nominal beam energy
Aperture radius: 13.0 mm
Integrated gradient: 14.3 Tm/m
Nominal gradient: 67.1 T/m
Nominal current: 35.3 A
Nom. power consumption: ~ 400 W
Iron length: 200 mm
Magnetic length: 213 mm
Total length: 270 mm
Magnet width: 390 mm
Magnet total mass: 180 kg
Space available for BPM: 109 (74) mm
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DBQ Magnetic Field Calculations
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DBQ Magnetic Field Quality
Gradient homogeneity along the x-axis
0.0E+00
5.0E-05
1.0E-04
1.5E-04
2.0E-04
2.5E-04
3.0E-04
3.5E-04
4.0E-04
4.5E-04
5.0E-04
-12.5 -7.5 -2.5 2.5 7.5 12.5
x [mm]
dB
y/d
x w
rt G
0
2.50 GeV 2.42 GeV 2.31 GeV 2.08 GeV 1.50 geV 0.70 GeV
0.24 GeV GFR
Gradient homogeneity along the GFR boundary
-4.0E-04
-3.0E-04
-2.0E-04
-1.0E-04
0.0E+00
1.0E-04
2.0E-04
3.0E-04
4.0E-04
5.0E-04
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0
angle [degree]
d|B
|/d
r w
rt G
0
2.50 GeV 2.42 GeV 2.31 GeV 2.08 GeV 1.50 geV 0.70 GeV 0.24 GeV
Gradient homogeneity:
Better than 5 * 10-4 inside good-field-region (GFR)
GFR radius: 11 mm
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DBQ Magnetic Field Quality
Magnetic Field Quality
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DBQ Excitation Curve
0
10
20
30
40
50
60
70
80
90
0.0 0.5 1.0 1.5 2.0 2.5 3.0
Beam energy [GeV]
Gra
die
nt
[T/m
]
0.0%
1.0%
2.0%
3.0%
4.0%
5.0%
6.0%
7.0%
Sat
ura
tio
n [
%]
Theor. gradient Calc. gradient Series4 Saturation
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TBL Quadrupole
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Main Beam Quadrupoles MBQ
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15
MBQ Requirements and Constraints
Aperture and field requirements
– Magnetic length: between 350 and 1850 mm
– Field gradient: 200 T/m
– Aperture radius: 4 mm
Indirect water cooling
– Max. current density 3 A/mm2
Integrated pulsed (20 ms) H/V steering coils (2 mT)
Large number (4000)
– High reliability, very robust design, low MTBF
Small aperture, long structure
– High mechanical precision
– Tight manufacturing and assembly tolerances
– Good mechanical stability
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MBQ Design Parameters
Aperture radius: 4.00 mm
Integrated gradient: 70 (170, 270, 370 ) Tm/m
Nominal gradient: 200 T/m
Iron length: 346 (846, 1346, 1846) mm
Magnetic length: 350 (850, 1350, 1850) mm
Magnet width: < 200 mm
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17
MBQ Magnetic Field Calculations
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MBQ Gradient Homogeneity
Gradient homogeneity along the GFR boundary
-4.0E-04
-3.0E-04
-2.0E-04
-1.0E-04
0.0E+00
1.0E-04
2.0E-04
3.0E-04
4.0E-04
0.0 20.0 40.0 60.0 80.0 100.0 120.0 140.0 160.0 180.0
angle [degree]
d|B
|/d
r w
rt G
0 [%
]
Pure quadrupole Pure dipole
Gradient homogeneity:
Better than 4 * 10-4 inside good-field-region (GFR)
GFR radius: 2.5 mm
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MBQ Corrector Field Homogeneity
Gradient resp. dipole field homogeneity along the x-axis
0.0E+00
5.0E-05
1.0E-04
1.5E-04
2.0E-04
2.5E-04
3.0E-04
3.5E-04
4.0E-04
4.5E-04
5.0E-04
-3.0 -2.0 -1.0 0.0 1.0 2.0 3.0
x [mm]
dB
y/d
x w
rt G
0
0.00E+00
5.00E-02
1.00E-01
1.50E-01
2.00E-01
2.50E-01
3.00E-01
3.50E-01
4.00E-01
4.50E-01
5.00E-01
By
wrt
By(
0)
Pure quadrupole GFR Pure dipole
Dipole field homogeneity:
Better than 4 * 10-1 inside good-field-region (GFR)
GFR on x-axis: ± 2.5 mm
Strong sextupolar component (b3)
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Open Issues
Detailed cooling circuit study
– Long term reliability
– Heat dissipation into tunnel
– Cooling efficiency
– New insulation materials
Mechanical and thermal stability
– Thermal expansion
– Cooling flow induced vibrations
Manufacturing and assembly tolerances
– Small aperture
– Long and slim structure
– Large series prodution
– New technologies required
Magnetic measurements, vacuum chamber integration, corrector optimization
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Conclusions and Future Work
A preliminary design for the CLIC DB and MB quadrupoles has been presented
A classical and robust layout has been chosen to maximize reliability and machine availability
The proposed designs fullfill the basic requirements and constraints, in particular the required dimensional limitations
DB Quadrupoles:
– The ‘two-current' proposal (DB) seems to be feasible and a good alternative to individually powered quadrupoles
– Number of magnet per string has to be optimized in view of the longitudinal beam dynamics constraints
– Protoypes for TBL and study their performance
MB Quadrupoles:
– Future studies and work addressing open issues
– Prototype needed to verify design and to study stability of assembly