18
Shigemi Sasaki , Elizabeth Moog, Maria Petra •Magnetic Design Evaluation of performance •Magnetic Material Type and reason Radiation susceptibility

Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

  • View
    219

  • Download
    1

Embed Size (px)

Citation preview

Page 1: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Shigemi Sasaki, Elizabeth Moog, Maria Petra

•Magnetic Design

Evaluation of performance

•Magnetic Material

Type and reason

Radiation susceptibility

Page 2: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Magnet & Pole Dimensions

9.0

0

6.0

0

48.00

56.50

0.80

1.5

0

0.50 Magnet

Polechamfer 0.5 x 0.5

Pole

Magnet5.0

0

30.0°2

.00

2.00

44

.00

66

.00

Page 3: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Magnetic field lines

Page 4: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Permeability in the pole

Page 5: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Demagnetizing field next to pole

Page 6: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Demagnetizing field at edge of pole

Page 7: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Demagnetization Curves for N39UH

Page 8: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

LCLS Undulator Model

Model calculation was made by using RADIA.NdFeB magnets with Br=1.24 T, and Vanadium permendur poles were assumed for calculation.

Page 9: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Shin-Etsu NdFeB Grades

Page 10: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility
Page 11: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

LCLS Prototype UndulatorGap dependence of Bp and Beff

0.8

0.9

1.0

1.1

1.2

1.3

1.4

1.5

1.6

5.8 6.0 6.2 6.4 6.6 6.8 7.0 7.2 7.4 7.6 7.8 8.0 8.2 8.4 8.6

Gap [mm]

Bpe

ak &

Beff

[T

]

Bpeak [T]Beff [T]

Gap dependence of magnetic fieldNdFeB: Shin-Etsu N39UH

Page 12: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Gap dependence of magnetic field

Sm2Co17, Br=1.14 T

0.8

0.9

1

1.1

1.2

1.3

1.4

1.5

1.6

5.8 6.0 6.2 6.4 6.6 6.8 7.0 7.2 7.4 7.6 7.8 8.0 8.2 8.4 8.6

Gap [mm]

Bp

eak &

Bef

f [T

]

Bpeak [T]

Beff [T]

Page 13: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Gap dependence of magnetic field

NdFeB vs SmCo

0.8

0.9

1

1.1

1.2

1.3

1.4

1.5

1.6

5.8 6 6.2 6.4 6.6 6.8 7 7.2 7.4 7.6 7.8 8 8.2 8.4 8.6

Gap [mm]

Bef

f [T

]

Beff [T]

Beff SmCo

Page 14: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Considerations of SmCo vs NdFeB

• SmCo is known to have a greater resistance to radiation-induced demagnetization than NdFeB, and the Sm2Co17 variety is better than SmCo5.

• Higher coercivity has been found to correlate with higher resistance to radiation damage.

• A new grade of NdFeB magnet (HILOP by Hitachi) has a higher coercivity than standard NdFeB. We estimate that the higher coercivity might make a difference of 6% in the radiation dose needed to cause a 1% decrease in the field.

• Using SmCo instead makes a bigger difference: Sm2Co17 gives a damage level of less than 0.2% out to as high as they exposed the magnets. Exposure to cause 1% loss in NdFeB ranged from ~23 to 30 x 10^13 electrons (at 2 GeV), whereas the dose to SmCo went out to 40, 65, or 175 x 10^13 electrons. So on that scale SmCo wins hands down [1].

[1] T. Bizen, T. Tanaka, Y. Asano, D.E. Kim, J.S. Bak, H.S. Lee, H. Kitamura, Nucl Instrum. Meth. Phys. Res. A467-468 (2001) 185.

Page 15: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Coercivity & Dose

22

24

26

28

30

32

1200 1400 1600 1800 2000 2200 2400

Data 1

dose

y = 14.991 + 0.0062007x R= 0.99672

dose

Page 16: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

NdFeB

Magnet grade Dose for 1% loss (10^13 electrons)

Coercivity (kA/m) Br (T)

N44 23 1273 1.36

N35 27 1989 1.17

N32 30 2387 1.11

 

“Demagnetization of undulator magnets irradiated high energy electrons”, T. Bizen, T. Tanaka, Y. Asano, D.E. Kim, J.S. Bak, H.S. Lee, H. Kitamura, Nucl Instrum. Meth. Phys. Res. A467-468 (2001) 185.

    Br (T) Coercivity (kA/m)

Hitachi HS-43EH 1.26 – 1.34 1989

Shin-Etsu N42SH 1.27 – 1.32 1671

Page 17: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Reasons for Our Choice

Does the extra resistance of as-purchased SmCo make a practical difference in the longevity of the magnets in LCLS so that it is worth going that way?

Look at how long it might take for damage:Say it takes 3x10^14 electrons at 2 GeV to lose 1% in NdFeB field.That’s 5x10^-5 C, or 50 microcoulomb.If we can only tolerate 0.01% loss in strength, then we can only tolerate 500 nC.The beam will be up to 1 nC per pulse, with pulses at 120 HzAssuming a loss rate of 10^-6 of the beam, how long to damage magnets? current x time x loss rate = 120 nA x time x 10^-6 = 500 nC gives time = 4 x

10^6 sec = 1000 hrs = 1.5 monthThe SmCo might last 15 times longer (0.2% loss at ~100 x10^13 electrons

instead of 1% loss at 30 x 10^13 electrons), which would take the time to 22 months, but that’s still not good enough. The beam loss rate in the undulators really has to be infinitesimal.

Page 18: Shigemi Sasaki, Elizabeth Moog, Maria Petra Magnetic Design Evaluation of performance Magnetic Material Type and reason Radiation susceptibility

Continued

• SmCo magnets are slightly weaker than NdFeB, by about 10%. For a 30-mm-period undulator, that would translate into a gap difference of nearly 1 mm.

• SmCo magnets are more expensive, by about a factor of 2.

• We have not yet bought a set of SmCo magnets, so we don’t know first-hand how uniform the quality is, though Shin-Etsu claims they could meet the same requirements with SmCo as they do with NdFeB.