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Quench Stability against Beam-loss in Superconducting Magnets at - - PowerPoint PPT Presentation

11/ 7/ 2003@KEK Quench Stability against Beam-loss in Superconducting Magnets at the 50 GeV Proton Beam Line for the J- PARC Neutrino Experiment Yosuke Iwamoto, Nobuhiro Kimura, Toru Ogitsu, Hirokatsu Ohhata, Atsuko Ichikawa, Tatsushi Nakamoto


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11/ 7/ 2003@KEK

Quench Stability against Beam-loss in Superconducting Magnets

at the 50 GeV Proton Beam Line for the J- PARC Neutrino Experiment

Yosuke Iwamoto, Nobuhiro Kimura, Toru Ogitsu, Hirokatsu Ohhata, Atsuko Ichikawa, Tatsushi Nakamoto and Akira Yamamoto, KEK Kenji Tanabe, University of Tokyo

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Contents Investigate the quench stability of the cables using J-PARC neutrino beam line In case of 50GeV-10W/point beam loss (Acceptable beam loss in view of shielding and maintenance) Calculate heat load for a 10 W/point beam loss in the cable by MARS code

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Iron yoke collar Plastic spacer Coil Corrector Beam tube X Z 330 cm X Y 55 cm

50GeV-10W beam

Heat load will be up to 20 kJ/m3/pulse. Heating of 0-40 kJ/m3/pulse was used in experiment and the quench simulation. Heat Load Simulation using MARS code

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Contents Investigate the quench stability of the cables using J-PARC neutrino beam line In case of 50GeV-10W/point beam loss (Acceptable beam loss in view of shielding and maintenance) Calculate heat load for a 10 W/point beam loss in the cable by MARS code is 20kJ/m3/pulse.

Using Heating of 0-40 kJ/m3/pulse

Measurements

  • f temperature rise of the cable
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Experiment

10 ms current 3.6 s The cable used the same structure of superconducting magnet. It was made of CuNi in order to generate Joule heating.

Heat load (kJ/m3/pulse) 8, 14, 20, 28, 37 Current (A) 30, 40, 50, 60, 70

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Cross section of the cable Specimen

  • verview
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28 kJ/m3/pulse heat load. 0.46 K temperature rise.

Experimental result

  • Temp. rise is proportional to heat load.

20 kJ/m3/pulse for a 50GeV-10W loss Instantaneous temp. rise = 0.25 K

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Contents Investigate the quench stability of the cables using J-PARC neutrino beam line In case of 50GeV-10W/point beam loss (Acceptable beam loss in view of shielding and maintenance) Calculate heat load for a 10 W/point beam loss in the cable by MARS code is 20kJ/m3/pulse

Using Heating of 0-40 kJ/m3/pulse Quench stability simulation.

Measurements

  • f temperature rise of the cable

is 0.25 K for a 20kJ/m3/pulse loss.

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Quench Stability Simulation

dt dT T AC gA Pq dx dT T k dx d A

p s

) ( ) ( = + −      

) (

b s

T T h q − =

h: heat transfer coefficient to SHe=2000 W/m2K Tb: SHe bath temperature a: strand diameter

Heat balance equation

A: the overall cross section K(T): thermal conductivity of conductor P: strand’s wetted perimeter qs: heat transfer to SHe g: Joule heating in conductor Cp(T): volumetric specific heat of conductor

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P/πa ~ 0.4 (the actual cable) 120 kJ/m3/pulse heat load (for a 50GeV-60W beam loss) may be acceptable. 20 kJ/m3/pulse heat load is OK (for a 50GeV-10W beam loss)

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Summary

Calculation result by MARS which simulate the actual magnet in the J-PARC neutrino beam line Heat load in coil will be up to 20 kJ/m3/pulse for a 10W/point beam loss

Instantaneous temp. rise in the cable = 0.25 K Not induce a quench. At least, 120 kJ/m3/pulse heat load for a 50GeV-60W beam loss may be acceptable. Experimental result Quench simulation result