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Technologie des aimants à tres haut champs et applications 1 GHz Dr. Rainer Kümmerle, Daniel Baumann
30ème Journée Utilisateurs RMN Bruker; Maison de la Chimie, Paris Mardi 29 Novembre 2016
1 GHz Aeon at NZN Bayreuth
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Niob-Titanium Wire Production
Cold extrusion from 1 m length to 20’000 m
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NbTi & Nb3Sn “wire” samples at intermediate drawing stage
NbTi, 36 Filaments Nb3Sn, 40,000 Filaments
NbTi, 8.670 Filaments
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(NbTaTi)3Sn wire with ~ 40.000 filaments
199 filament bundles
199 filaments in each bundle
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Low Temperature Superconductors (LTS)
NbTi:
Critical temperature TC : 9.6 K
Highest magnetic field: ~11 T
(useful up to fields of ~400 MHz)
Nb3Sn:
Critical temperature TC : 18 K
Highest magnetic field: ~23…26 T
(useful up to fields of ~1 GHz)
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Nb3Sn production and processing: cold extrusion
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Low Temperature Superconductors (LTS)
Niobum-Bronze wire, easy to bend/wind
Niobum-Bronze wire with glass fibre
insulation
Reacted (heat-treated) Nb3Sn wire,
brittle like ceramics
1.2 x 1.8 mm ~ 40’000 filaments
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Nb3Sn production & processing: winding & reaction process
• Copper (heatload, quench protection)
• Bronze; Cu with up to 16% Sn & 0.3 % Titanium
• Niobium
• Tantalum
• Glass fiber insulation
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Nb3Sn production & processing: winding & reaction process
Desizing:
Glassfibre mesh insulation is pulled over the wire, potato starch is used to lubricate.
Before heat treatment the starch needs to be removed. This is achieved by repeated heating
and vacuum pumping.
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Nb3Sn production & processing: winding & heat treatment process
• The wound Nb3Sn coils are heat treated in a ca. 2
weeks process
• The process takes place in a high vacuum oven
which transfers heat via internal radiation plates to
the wound coils
• Depending on the wire manufacturer, the wire
diameter and the shape of the wire the heat
treatment process needs to be adapted
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Mechanical forces on wires
• Copper
• Bronze
• Niobium
(Tensile strength: 125 MPa)
• Tantalum
(Tensile strength: 170…300 MPa)
• The different materials within the wire need to have very similar expansion coefficients
(from RT up to ~700°C and later from RT down to -269°C)
• Requires extremly robust coil former
• The coil former design is optimized to neither produce additional forces on wire nor to allow for
empty space
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Mechanical forces on wire
In a charged superconducting coil forces point in different
directions depending on position:
• Radial Force Diameter-dependent pressure/stress
(hoop-stress, up to 200 MPa)
• Axial Force transverse stress on wire
200 MPa = 2000 bar or ~1973 atm
(20400 m water column)
For comparison: 30 atm or 300 m is a typical lower dive level
for larger submarines
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16 17 18 19 20 21 22 23 24 250
100
200
300
400
T = 4.2K
T = 4.2K
T = 2.2K
16%Sn
16%Sn
14%Sn
(NbTaTi)3Sn
(NbTaTi)3Sn with high Sn content
(NbTaTi)3Sn with high Sn content T=2.2K
21T
Jc,o
vera
ll (
A/m
m2)
0H (Tesla)
700 800 900 1000
1 GHz
Proton Resonance Frequency (MHz)
Wire Technology: bronze wire with high Sn content
1.83x1.22 mm2
28000 Filaments
f Filaments = 4.8 m
Cu-16%Sn-Ti Bronze
Increased Sn content Higher Critical Current Jc
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Temperature T
T=const.
B=const.
max. jc(4.2K, 12T)
Magnetic field B
Critical Surface
Current density jc
4.2 K
12T
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Key Bruker UHF Magnet Technologies
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Active shielding (3rd generation)
Field coil Shielding coil
External Disturbance Suppression (EDS™)
Active refrigeration Aeon™ technology
2K cooling
Advanced LTS Superconductors
UHF Coil technology
Bo
Key UHF Technologies: High current designs and rectangular wire
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High current design
• rectangular wire • conductor area = 4 mm²
IM = 2 · Io
+ Bo
Low current design
+ Bo
IM = Io
• round wire • conductor area = 2 mm²
Advantages of Rectangular UHF LTS
• Higher current results in larger wire cross sections
• Better winding chamber filling factor
• Less insulation material in winding chamber
• Better control of forces
• Enables highest fields
• Enables smaller magnets
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NbTi-conductor (NbTaTi)3Sn-conductor
Nb
(NbTaTi)3Sn Bundle
2 mm
1 m
m
Cu
UltraStabilized™ 2 Kelvin sub-cooling: used today for 850 MHz to 1.2 GHz
• Long term stable magnet
• Highest field strengths
• Increased magnet stability
• Higher safety margins
• Lowest drift rates
• Easy helium refills
• Compatible with new Aeon™ & HTS technologies
• Patented technology
• Pioneered by Bruker
• Proven track record
• Over 230 systems installed
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UltraStabilized™ technology delivering
unique performance, stability and safety
Thermal Barrier
Joule-Thompson
Cooling Unit
Superconducting
Magnet Coil
Aeon Active-Refrigeration: no compromise on High-Resolution NMR Performance He-Re-Liquefaction for 2K sub-cooled magnets
• Sub-cooled LHe bath at same pressure of 1.05 bar as the 4.2K bath
• Low pressure (below 30 mbar) limited to the JT cooling unit maintained by pumping
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Subcooled helium gas
Sub-cooling Pump in BMPC II unit
Plo
w
Phig
h
He compressor
He g
as r
etu
rn lin
e
• He gas exhausted from the pump at room temperature and fed back to a PTC
• Recovered He gas re-liquefied by the PTC
• Thermal shield cooled by the 1st stage of the PTC (N2 free, no nitrogen vessel)
No Cryogen consumption during normal operation
J-T Unit
PTC
Bruker UHF Magnet Milestones
• 1992 First 750 MHz magnet
• 1995 First 800 MHz NMR magnet
• 1998 First 750 MHz wide bore magnet
• 2001 First 800 MHz actively shielded magnet
• 2004 First 850 MHz WB shielded magnet
• 2004 First 900 MHz actively shielded magnet
• 2006 First 800 MHz single-story shielded magnet
• 2006 First 950 MHz actively shielded magnet
• 2009 First 900 MHz WB shielded magnet
• 2009 First 850 MHz single-story shielded magnet
• 2009 First 1000 MHz magnet (unshielded)
• 2012 First Single-Story Aeon 800 MHz WB
• 2013 First Single-Story Aeon 900
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750
Bruker UHF Magnets Today- the state of the art: - Actively shielded (3rd generation) - Aeon closed loop cooling (LN2-free, no LHe boil-off) - Persistent, homogeneous, ultra-stabilized
Aeon 950 54mm single-story NMR magnet
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Aeon 1 GHz 54mm NMR Magnet
Aeon 21 T 11cm FTMS/MRI Magnet
Aeon 950 MHz 5mm TCI: Water Suppression
2mM Sucrose in H2O:D2O 90:10
Resolution: 11%
Hump: 8.3 / 29.8 Hz
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10 9 8 7 6 5 4 3 2 1 0 ppm
5.385.405.425.44 ppm
Aeon 950 MHz 5mm TCI: 15N detection
15N detected refocused INEPT
C/N-labeled ubiquitin
Adiabatic 13C (Chirp, 48 kHz sweep) CPD decoupling.
NS = 32, expt. Time 60 seconds
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105110115120125130 ppm
Aeon 950 MHz 5mm TCI
C/N-labeled ubiquitin
1H-15N sofast-HMQC
NS = 2
TD = 1k x 128
Expt. Time 18 seconds
Vertical projection: 15N detected INEPT
Horizontal projection: C & N decoupled excitation
sculpting
25
ppm
7.27.47.67.88.08.28.48.68.89.09.29.49.69.8 ppm
105
110
115
120
125
130
Aeon 950 MHz 5mm TCI
C/N-labeled ubiquitin
3D (H)CCH-TOCSY 2D CH plane
NS = 4
TD = 3k x 256
Mixing = 9ms @ 12.5 kHz
Expt. Time 20 minutes
26
ppm
-0.55.5 5.0 4.5 4.0 3.5 3.0 2.5 2.0 1.5 1.0 0.5 0.0 ppm
10
20
30
40
50
60
70
Aeon 950 MHz 5mm TCI: 15N detection
C/N-labeled ubiquitin
15N detected 3D CBCACON
NS = 16
TD = 2k x 64 x 80
D1 = 1s
Expt. Time: 30 hours
3D and NCO / NCaCb projections shown
27
ppm
105110115120125130135140 ppm
15
20
25
30
35
40
45
50
55
60
65
70
ppm
105110115120125130135140 ppm
168
169
170
171
172
173
174
175
176
177
178
179
d(N)
d(CO)
d(N)
d(C)
Aeon 950 MHz 5mm TCI: 15N detection
C/N-labeled ubiquitin
15N detected 3D (h)CCCON
NS = 16
TD = 2k x 64 x 96
D1 = 1s
Expt. Time: 37 hours
3D and NCO / NCC projections shown
d(N)
d(N)
d(C)
d(CO)
28
ppm
105110115120125130135140 ppm
15
20
25
30
35
40
45
50
55
60
65
70
ppm
105110115120125130135140 ppm
168
169
170
171
172
173
174
175
176
177
178
179
• Active shielding reduces space requirements by > one order of magnitude
• Aeon 1 GHz magnets leverage advanced BEST superconductors
• Active refrigeration eliminates LN2, reduces LHe boil-off essentially to zero
New GHz-class magnet, novel Cryoprobes, 111 kHz MAS probes, and new
NMR methods expand frontiers in structural biology, membrane protein and intrinsically disordered protein (IDP) research
ENC 2016 Announcement: World's first shielded Aeon 1 GHz System installed
Aeon 1 GHz at Research Center for Bio-Macromolecules at University of Bayreuth
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1 GHz 5mm TCI: Water Suppression
2mM Sucrose in H2O:D2O 9:1
Resolution: 10%
Hump: 9.7 / 16.7 Hz
Composite pulse & crusher gradient presat
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10 9 8 7 6 5 4 3 2 1 0 ppm
5.395.405.415.42 ppm
1 GHz 5mm TCI: 13C RF power handling
2mM Sucrose in H2O:D2O 9:1
1H-13C HSQC
NS = 2
TD 8k x 256
AQ 400ms
Adiabatic CPD decoupling
31
ppm
3.53.63.73.83.94.04.14.24.3 ppm
60
62
64
66
68
70
72
74
76
78
80
82
1 GHz 5mm TCI: 13C RF power handling
2mM Sucrose in H2O:D2O 90:10
1H-13C HSQC
AQ 400ms
Adiabatic CPD decoupling
2D HSQC 1H projection
1D 1H spectrum
32
1 GHz 5mm TCI: CC-TOCSY
C/N-labeled ubiquitin
13C detected CC-TOCSY
NS = 16
TD = 4k x 128
Mixing = 20ms @ 13.5 kHz
Expt. Time 40 minutes
33
ppm
510152025303540455055606570 ppm
10
20
30
40
50
60
70
1 GHz relaxation-optimized 3D
C/N-labeled ubiquitin
3D BEST-HNCO
NS = 2
TD = 1k x 48 x 96
D1 = 100ms
Expt. Time 40 minutes
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1 GHz relaxation-optimized 3D
C/N-labeled ubiquitin
3D BEST-HNCO
NS = 2
TD = 1k x 48 x 96
D1 = 100ms
NUS 12.5% with CS processing
Expt. Time: 5 minutes!
(traditional sampling: 40 minutes)
35
1 GHz relaxation-optimized 3D
C/N-labeled ubiquitin
3D BEST-TROSY-HNCOCACB
NS = 2
TD = 1k x 64 x 256
D1 = 200ms
Expt. Time: 3 hours 46 minutes
36
1 GHz relaxation-optimized 3D
C/N-labeled ubiquitin
3D BEST-TROSY-HNCOCACB
NS = 2
TD = 1k x 64 x 256
D1 = 200ms
NUS: 12.5 % with CS processing
Expt. Time: 28 minutes
(traditional sampling: 3.75 hours)
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Acknowledgements
• Daniel Baumann
• Gerhard Roth
• Patrick Wikus • Ruedi Gaisser
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www.bruker.com
For research use only. Not for use in diagnostic procedures. Copyright © 2010 Bruker Daltonics. All rights reserved.
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