generation of strong external magnetic field at luli ......outline pulsed power system coil able to...
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Albertazzi Bruno
Magnetic meeting 23-24 April, Rochester
Generation of strong external
magnetic field at LULI
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Outline
Pulsed power system
Coil able to generate up to 40 T B-field (two 5 mm diameter access)
Coil able to generate up to 15 T B-field (three 1.1 cm diameter access)
Perspectives
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Motivation
Build a plateform able to generate strong external magnetic field (> 10 T)
Huge volume ( ≥ cm3), constant over long time (≥ µs)
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Motivation
Plasma in
expansion
Poloidal Magnetic
Field (Bpol)
(Bpol) Spherical expansion stopped when σ ~ 1
𝑅𝑐𝑜𝑙𝑙 𝑐𝑚 ~0,8[𝑓𝐸𝐿 𝐵02]1/3
Collimation radius
Laser
Collimation time given by : 𝜏𝑐𝑜𝑙𝑙~𝑅𝑐𝑜𝑙𝑙/𝑣𝑒𝑥𝑝 with 𝑣𝑒𝑥𝑝 = 4,6.107 𝐼141/3
𝜆µ𝑚2/3
(𝑐𝑚. 𝑠−1)
To magnetically collimate a
jetlike flow with radius of
few mm,
B > 10 T applied for t > 10
ns Coll
imat
ion r
adiu
s (m
m)
Magnetic Field (T) Magnetic Field (T)
Coll
imat
ion t
ime
(ns)
A. Ciardi et al., Phys. Rev. Lett 110, 025002 (2013)
Build a plateform able to generate strong external magnetic field (> 10 T)
Huge volume ( ≥ cm3), constant over long time (≥ µs)
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Our method
Pulsed power system @ LULI
High current Generation :
- Build by HZDR
- 250 kA maximum
- Available energy : 32 kJ
- Short rise time(~µs)
- Ignitron switch
Pulser
Experimental
chamber Transmission
line
[B. Albertazzi et al., Rev. Sci. Instru 84, 043505 (2013)]
Patent: Device for magnetising laser plasma by means of a pulsed magnetic field
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Our method
Pulsed power system @ LULI
Pulser
Experimental
chamber Transmission
line
[B. Albertazzi et al., Rev. Sci. Instru 84, 043505 (2013)]
Patent: Device for magnetising laser plasma by means of a pulsed magnetic field
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Coil developed by the LNCMI
Laser
Diagnostics
access
Top view Our Method implies :
- Coil in air : NO DEBRIS
- Reduced thermal load
- Drastic diminution of risks of
arcing between experimental
chamber and transmission line
[B. Albertazzi et al., Rev. Sci. Instru 84, 043505 (2013)]
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Coil developed by the LNCMI
2 access of 5 mm diameter:
Laser and diagnostics
Magnetic field up to 40 T
Constant in a huge volume (cm3)
Easily synchronisable with the laser
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Coil developed by the LNCMI
Rise time to first peak : ~ 176 µs
I/B~300 A/T, for 40 T Imax~ 12 kA
Discharge without current
limiter
Discharge with current limiter
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Coil developed by the LNCMI
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Coil developed by the LNCMI
Time following pulsing of the coil (s)
Me
an
co
il t
em
pe
ratu
re (
K)
Evaluation of the repetition rate in an experimental manner at 20 T and comparison
with theoretical calculations :
Repetion rate of the order of 10-15 min at 20 T and of 30-45
min at 40 T : compatible with High powers Laser Facility
avoid cumulative effects
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Conclusion
Magnetic field up to 40 T
Constant in a huge volume (cm3)
Constant in time (> 5 µs), with less than 2% variation
However:
Restriction about access to the plasma
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Coil developed by the HZDR
Laser and
diagnostics access
Inside the coil
3 access of 1 cm diameter
Magnetic field up to 15 T (will be improved for future experiments)
Constant in a huge volume (> cm3)
Easily synchronisable with the laser
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Coil developed by the HZDR
Ma
gn
etic
fie
ld (
T)
(mm)
(mm
)
Constant volume > 1cm3
Constant over 10s of µs duration
Simulation of the coil
0 50 100 1500
2
4
6
8
10
Time (µs)M
ag
net
ic f
ield
(T
)
Rogowski measurement
31.5 kA
Constant over µs
duration
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Conclusion
Magnetic field up to 15 T (will be improved)
Constant in a huge volume (cm3)
Constant in time (> 20 µs), with less than 2% variation
More access for laser and diagnostics X-ray radiography coupled
with optical diagnostics
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Perspectives
Increase the available energy of the pulse power system:
Design of the coil less restrictive
Developmnent of a coil allowing to have a transverse magnetic field
(20 T) compared to the drive laser axis together with the x-ray
radiography (HZDR collaboration)
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Acknowledgements
A. Ciardi3,4, M. Nakatsutsumi1, T. Vinci1, J. Béard5, S. Bonito6,7, J. Billette5, M. Borghesi8,9, Z.
Burkley1, S.N. Chen1, T. E. Cowan10,11, T. Herrmannsdörfer7, D. P. Higginson1, F. Kroll10,11, S. A.
Pikuz12,13, K. Naughton8, L. Romagnagni1, C.Riconda1, G. Revet1, R. Riquier1,15, H-P. Schlenvoigt11, I.
Yu. Skobelev12, A. Ya. Faenov12,16, A. Soloviev17, M. Huarte-Espinosa18,19, A. Franck18, O. Portugall5,
H. Pépin2, J. Fuchs1,17
E. Falize2,3, A. Pelka4, F. Brack4, F. Kroll4, R. Yurchak1 , E. Brambrink1, P. Mabey1, N. Ozaki6, S.
Pikuz7,8, L Van Box Som2,3, J. M. Bonnet-Bidaud3, J. E. Cross9, E. Filippov7,8, G. Gregori9, R.
Kodama10, M. Mouchet11, T. Morita12, Y. Sakawa10, R.P. Drake,5, C. C. Kuranz5, M. J.-E. Manuel13, C.
Li14, P. Tzeferacos15, D. Lamb15, U. Schramm4 and M. Koenig1,6