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Simulation Study of Solenoidal-Lithium Lens Channel

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Presentation on theme: "Simulation Study of Solenoidal-Lithium Lens Channel"— Presentation transcript:

1 Simulation Study of Solenoidal-Lithium Lens Channel
K. Lee, D. Cline, A. Garren March 02, 2011 MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

2 Previous Studies with Lithium lens
Curved Li lens (~2004-current) by Y. Fukui Cooling Ring studies (~ ) using Li lens by A. Garren and Y. Fukui Initial engineering considerations for a liq. Li lens (2008) with some inputs from J.P. Morgan and T. Leveling at Fermilab and BINP papers Achieved some cooling with long periodic 3 cm length Li lens channel (2009) MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

3 MAP Winter Meeting at JLab
Final Cooling Stages MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

4 MAP Winter Meeting at JLab
Li Lens Properties Strongly focusing Low Z material for ionization cooling B field ~ 10 T at surface low  region MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

5 Fermilab Solid Li Lens (Recent Design)
D 2.0 cm x L 15 cm Induction Coils J. Morgan Lens Upgrade Note MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

6 Cooling in an ideal Li Lens
azimuth. B I 500 kAmps Beam focusing parameter in the azimuthal B field (cm, MeV/c, T) Equilibrium beam parameters (cm, MeV/c, T) (cm, T) MAP Winter Meeting at JLab Feb 28-Mar 4, 2011 V. Balbekov, Aug. 2006

7 MAP Winter Meeting at JLab
Channel with One 10 cm x 135 cm Lens Comparison between 10 T and 20 T exit solenoid MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

8 Series of 9 cm Li lens Channel of 300 cells
G=6.2 T/cm RF=54 MV/m MAP Winter Meeting at JLab Feb 28-Mar 4, 2011 K. Lee, D. Cline, A. Garren

9 Series of 9 cm Li lens Channel of 300 cells
MAP Winter Meeting at JLab Feb 28-Mar 4, 2011 K. Lee, D. Cline, A. Garren

10 MAP Winter Meeting at JLab
Only the lenses are simulated. Ideal matrix is used instead of matching sections. Schematic and idea of the channel (V.Balbekov, MCD Workshop, Dec. 2009) Main parts of the channel: Blue – solenoid coils Red -- Li lenses Green – 200 MHz cavities Transition from high to low field region is adiabatic itself. Li lens should provide the adiavatic transition from (+) field to (-) one Li rod should have a special form to provide the adiabaticity (example) With solenoid field B and lens gradient G, beta – function is: Adiabaticity condition (Palmer) Gray – fringe regions where a special study is needed ? MAP Winter Meeting at JLab Feb 28-Mar 4, 2011 V.Balbekov Mar 18, 2010

11 MAP Winter Meeting at JLab
Only the lenses are simulated. Ideal matrix is used instead of matching sections. Solenoid field Blue: high-field solenoid coils, right-hand part Pink: a half of Li lens (schematically). Volume of diameter 30 cm is provided for it Axial field in the solenoid axes. Maximal value 50 T Transport 4 Tesla solenoid has inner radius 60 cm. 02c_rod.pdf Other coils were considered as well (shape, size, etc.). In all the cases, transition from high to low field is adiabatic (at proper current density), and required beta-function is provided by optimization of the Li lens. Conclusion: design of this assembly is an engineering problem, primarily. MAP Winter Meeting at JLab Feb 28-Mar 4, 2011 V.Balbekov Mar 18, 2010

12 2-D Axial Field Map by COMSOL
50 cm 30 cm 20 cm J = 3.18 108 A/m2 60 cm 15 cm 2 m MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

13 MAP Winter Meeting at JLab
Li Lens Profile 100% 90% 50% 14% MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

14 Solenoidal Li Lens Channel with ICOOL
MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

15 Solenoidal Li Lens Channel with ICOOL
MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

16 MAP Winter Meeting at JLab
Summary Achieved some cooling with Balbekov’s suggestion Complete the simulation in the next 9 months Add more realistic features Adjust the solenoid coils Adjust the Li lens length Windows MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

17 Liquid Li Lens Outstanding Issues
Mechanical fracture from current pulsing at > 500 kAmps per pulse Heat removal; achieved by rapid flow Magnetic skin depth at faster than a few Hz rate MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

18 Liquid Li Lens Development at BINP
The Li lens work by Dr. Silvestrov et. al at BINP was for use at the Tevatron anti-proton source (accord w/ Fermilab for run II) and at CERN. The lens survived < 100k pulses at 7.5 T (design was 10M and 13 T). Shock waves in the Li and cracking of the Ti septum. MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

19 Observed Fermilab Li Lens Lifetime
B grad (T/m) Avg. Life Time (Pulses) 1,000 <500,000 (1.9 wk) 900 1,000,000 (3.8 wk) 800 3,000,000 (5.7 wk) 740 9,000,000 (17 wk) 700 >10,000,000 (19 wk) J. Morgan Lens Upgrade Note MAP Winter Meeting at JLab Feb 28-Mar 4, 2011

20 Initial Mechanical Design
D 2.54cm  L 30cm Outer tube for heated oil above 200 C Double layered tubes for liquid Li and heated oil MAP Winter Meeting at JLab Feb 28-Mar 4, 2011


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