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MICE Absorber cryostat Forces and power dissipation - for normal operation and during a magnet quench Elwyn Baynham James Rochford MICE Meeting November.

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Presentation on theme: "MICE Absorber cryostat Forces and power dissipation - for normal operation and during a magnet quench Elwyn Baynham James Rochford MICE Meeting November."— Presentation transcript:

1 MICE Absorber cryostat Forces and power dissipation - for normal operation and during a magnet quench Elwyn Baynham James Rochford MICE Meeting November 2003

2 Outline Magnet Forces and Quench Issues »Scope –To review the interactions between the magnet system and the H2 absorber units –Magnet system brief overview – focus coils and absorber geometry – separation of modules – not all latest geometry –Magnetic Forces l Static - schematic of forces on coils – internal/external – force management – interaction with absorber l Quench – worst case unbalanced forces – management – interaction with absorber –Quench – present eddy currents,forces,power generated in absorber bodies and windows – for both flip and solenoid mode –Review Impact on absorber design and safety

3 Operational forces 183T228.5T Internal force restraint Suspension -internal axial force restraint External axial force restraint Between cryostats Nett 45T LH Flip mode 240MeV/c,b=43cm Nett 60T Nett 7.9T (Forces for outer most pair of flip coils)

4 Operational forces 146T99T Internal force restraint Suspension -internal axial force restraint External axial force restraint Between cryostats Nett 47.4T LH Solenoid mode 200MeV/c,b=7cm Nett 74.9T Nett 1.2T (Forces for outer most pair of flip coils)

5 Magnet Quench 2d Quench model

6 Magnet Quench Current rundown during a quench for 51H with no protection resistance

7 Magnet Quench Eddy current distribution in holders and windows 2s into a quench whilst operating in 240MeV/C,Beta=43cm mode Eddy current distribution in windows in flip mode

8 Magnet Quench Power dissipated in the inner vessel windows during a quench in 240MeV/C,Beta=43cmm mode

9 Magnet Quench Power dissipated in the inner vessel bodies during a quench in 240MeV/C,Beta=43cmm mode

10 Magnet Quench Force on the inner vessel windows during a quench in 240MeV/C,Beta=43cm mode

11 Magnet Quench Using expression We can estimate the peak stress in the window

12 Magnet Quench Model changed to look at the effect of offsetting a window axially

13 Magnet Quench Force on the inner vessel bodies during a quench in 240MeV/C,Beta=43cm mode with the vessels offset axially by 5mm

14 Magnet Quench Eddy current distribution in holders and windows 2s into a quench whilst operating in solenoid mode -200MeV/C,Beta=7cm Eddy current distribution in windows For Solenoid mode

15 Magnet Quench Power dissipated in the inner vessel windows during a quench for solenoid mode -200MeV/C,Beta=7cm

16 Magnet Quench Power dissipated in the inner vessel bodies during a quench for solenoid mode -200MeV/C,Beta=7cm

17 Magnet Quench Force on the inner vessel windows during a quench for solenoid mode -200MeV/C,Beta=7cm

18 Conclusions –Magnetic Forces l Static – internal/external force management is well understood – no significant interaction with absorber l Quench – coil body forces understood and controlled within magnet cryostat –Quench –eddy current l forces on windows very small cf vacuum/liquid loads l power generated in absorber bodies and windows will not cause significant pressure rise/liquid boil off –Impact on absorber design and safety –– no special design requirements for magnet interactions


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