Progress on the MICE Cooling Channel Magnets - PowerPoint PPT Presentation

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Progress on the MICE Cooling Channel Magnets

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AC losses induced by a quench do not appear to be a factor, except from mandrel heating. ... Coupling Coefficients between Magnet Circuits and Various Mandrels ... – PowerPoint PPT presentation

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Title: Progress on the MICE Cooling Channel Magnets


1
Progress on the MICE Cooling Channel Magnets
  • Michael A. Green
  • Lawrence Berkeley National Laboratory
  • 28 June 2005

2
3D View of the MICE Cooling Channel
Coupling Magnet Cryostat
AFC Module
RFCC Module
Courtesy of S. Yang Oxford University
3
Three Quarter Section View of the MICE Cooling
Channel
Courtesy of S. Yang Oxford University
Coupling Coil
Focusing Magnet Coil
4
Half Section View of theMICE Cooling Channel
Liquid Hydrogen Absorber
Focusing Magnet Coil
201 MHz RF Cavities
Coupling Coil
Courtesy of S. Yang Oxford University
5
Cooling Channel Magnet Progress
  • The cooling channel consists of three AFC modules
    and two RFCC modules.
  • This report will discuss the progress made since
    the last meeting on the focusing magnet and the
    coupling magnet.
  • Progress on the tracker magnet (detector magnet)
    will not be presented. This information was
    presented on June 27th.

6
Focusing Magnet
7
The MICE AFC Module
Courtesy of S. Yang Oxford University
8
The Center of the MICE AFC Module
Gas He Pipe
Coil Cover Plate
S/C Coil 1
S/C Coil 2
LH2 Absorber
Hydrogen Window
LH2 Pipes
Safety Window
Magnet Mandrel
Liquid Helium Feed Pipe
Courtesy of S. Yang Oxford University
9
The Focusing Magnet Parameters
These are the worst cases based on p 240 MeV/c
and b 420 mm
10
Focusing Magnet Progress
  • Progress has been made on the focusing magnet
    quench protection system and in the power system
    for the magnets.
  • The quench simulations show that the focusing
    magnets can be passively quenched without a
    formal quench protection system.
  • The three focusing magnets can be connected in
    series. External diodes and resistors are used
    to control the voltages across the coils.

11
Focusing Magnet QuenchOne Magnet 3 in Series
12
250 A Focusing Magnet QuenchFlip Mode Non-flip
Mode
13
Focusing Magnet Mandrel Tafter a Quench in the
Flip Mode
  • Max T 51.9 K
  • Min T 4.41 K
  • Quench Time 4 s
  • Istart 250.8 A
  • 0.80
  • p 240 MeV/c
  • b 420 mm

Courtesy of H. Witte Oxford University
14
Focusing Magnet Mandrel Tafter a Quench in the
Non-flip Mode
  • Max T 41.7 K
  • Min T 4.69 K
  • Quench Time 4 s
  • Istart 130.3 A
  • 0.80
  • p 240 MeV/c
  • b 420 mm

Courtesy of H. Witte Oxford University
15
Focusing Magnet Mandrel Hot Spot Tas a Function
of Time
  • Max T 51.9 K
  • Min T 4.41 K
  • Quench Time 4 s
  • Istart 250.8 A
  • 0.80
  • p 240 MeV/c
  • b 420 mm

Quench back occurs.
Courtesy of H. Witte Oxford University
16
Focusing Magnet Power System
17
Coupling Magnet
18
The MICE RFCC Module
Courtesy of S. Yang Oxford University
19
Coupling Magnet Parameters
20
Coupling Magnet Progress
  • Progress has been made on the coupling magnet
    quench protection system and in the power system
    for the magnets.
  • The quench simulations show that the coupling
    magnets can be passively quenched without a
    formal quench protection system.
  • The two coupling magnets can be connected in
    series, but it may be better to power the two
    magnets separately. Cold diodes and resistors
    are used to control the voltages within the coils.

21
Coupling Magnet QuenchOne Two Magnets in Series
22
Coupling Magnet Quench6061-T6 and 1100-O Mandrels
23
Coupling Magnet Mandrel Tafter a Quench in the
Flip Mode
  • Max T 83.9 K
  • Min T 4.21 K
  • Quench Time 5 s
  • 0.92
  • p 240 MeV/c
  • b 420 mm

Courtesy of H. Witte Oxford University
24
Coupling Magnet Mandrel Hot Spot Tas a Function
of Time
  • Max T 83.9 K
  • Min T 4.21 K
  • Quench Time 5 s
  • 0.92
  • p 240 MeV/c
  • b 420 mm

Quench back occurs.
Courtesy of H. Witte Oxford University
25
Coupling Magnet Power System
26
Coupling between Magnet Circuits
27
Coupling Coefficients between Coils
Magnet Circuit Self Inductance and the Mutual
Inductances in the Flip Mode
Magnet Circuit Self Inductance and the Mutual
Inductance in the Non-flip Mode
Courtesy of H. Witte Oxford University
28
Conclusions from the Self and MutualInductance
Calculations
  • Every magnet circuit in MICE is coupled to every
    other magnet circuit in MICE.
  • The charging or discharging of one magnet circuit
    will affect every other magnet circuit, but the
    power supplies can handle the effect.
  • A quench of one magnet circuit will not drive
    other magnets normal by changing the currents too
    much. AC losses induced by a quench do not
    appear to be a factor, except from mandrel
    heating.

29
Coupling between Magnet Coil Circuits and other
Magnet Mandrels
30
Currents for Various Cases and theCoupling
Coefficients
Coil Currents for Various Cases where p 240
MeV/c and b 420 mm
Coil to Mandrel Coupling Coefficients for Various
Cases
Courtesy of H. Witte Oxford University
31
Heating of the Coupling Mandrelby a Focusing
Quench (Flip Mode)
Courtesy of H. Witte Oxford University
  • Max T 4.45 K
  • Min T 4.41 K
  • Quench Time 4
  • 0.0018
  • p 240 MeV/c
  • b 420 mm

A quench of the focusing magnet circuit is
unlikely to quench the coupling magnet in the
flip mode.
32
Heating of the Coupling Mandrel by a Focusing
Quench (Non-flip Mode)
Courtesy of H. Witte Oxford University
  • Max T 4.76 K
  • Min T 4.69 K
  • Quench Time 4 s
  • 0.0137
  • p 240 MeV/c
  • b 420 mm

A quench of the focusing magnet circuit may
quench the coupling magnet in the non-flip mode,
at high momenta.
33
Heating of the Focusing Mandrel by a Coupling
Quench (Flip Mode)
Courtesy of H. Witte Oxford University
  • Max T 6.30 K
  • Min T 4.22 K
  • Quench Time 5 s
  • 0.0813
  • p 240 MeV/c
  • b 420 mm

A quench of the coupling magnet circuit is likely
to quench the focusing magnet in either mode.
34
Coupling Coefficients between Magnet Circuits and
Various Mandrels
Courtesy of H. Witte Oxford University
The quench of a cooling channel magnet circuit is
unlikely to cause a quench of a tracker magnet.
A tracker magnet quench wont quench the channel
magnets.
35
Conclusions from the Magnet Coupling Calculations
  • A quench of a focusing magnet is unlikely to
    quench any other magnet except the coupling
    magnet at high muon momenta in the non-flip mode.
  • A quench of a coupling magnet is likely to quench
    the focusing magnet except at low muon momenta.
    A coupling magnet quench will not quench the
    tracking magnet.
  • A quench of the tracker magnet is unlikely to
    quench any of the other magnets in MICE.

36
Concluding Comments
  • Engineering progress has been made on all of the
    MICE magnets and their sub-systems.
  • Quench calculations show that the MICE focusing
    and coupling magnets will quench safely. It is
    probable that the detector magnets will also
    quench safely. This will be verified before the
    next meeting.
  • A coupling magnet quench will cause the focusing
    magnet to quench, but a quench of the other
    magnets is unlikely to cause a quench of other
    magnets in MICE.
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