p. m. grant mgb 2 – one year later. p. m. grant mgb 2 – one year later paul m. grant science...
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P. M. Grant
MgB2 – One Year Later
MgB2 – One Year Later
Paul M. GrantScience Fellow
Electric Power Research InstitutePalo Alto, California USA
Wire Development Already Well Underway!Wire Development Already Well Underway!
P. M. Grant
MgB2 – One Year Later
OPW’s
• Tomsic (HyperTech)• Sargent (Diboride)• Grasso (INFM-Genova)• Caplin (Imperial College)• Larbalestier (UW/ASC)• Christen (ORNL)• Suenaga (BNL)• Canfield (Ames)
P. M. Grant
MgB2 – One Year Later
Maybe It Wasn’t Missed!
MgB2 Specific HeatR. M. Swift and D. White,
J. Am. Chem. Soc. 79, 3641 (1957)
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.45
0.50
10 20 30 40 50 60
T (K)
Mo
lal C
P (
ca
l/K)
?39
?32
P. M. Grant
MgB2 – One Year Later
Wither Beyond MgB2?
• MgB2 appears to be the quintessential electron-phonon coupling superconductor
• A “tepid temperature” compound
• So far, one of a kind…end of the road?
P. M. Grant
MgB2 – One Year Later
PowerDevice Req’mts
T (K) H (T) Jc (A/cm2)
Motors/Generators
30 4 100,000
Transformers 30 2 80,000
Current Limiters
30 2 80,000
Cables 77 0.5 70,000
Dick Blaugher, NREL
P. M. Grant
MgB2 – One Year Later
Is LN2 Necessary?
How far to Lq N2
0.0%
20.0%
40.0%
60.0%
80.0%
100.0%
0 10 20 30 40 50 60 70
Temperature
Ho
w f
ar
to L
q N
2 f
rom
Lq
He
Energy Consumption normalised at 4K
0.00
0.20
0.40
0.60
0.80
1.00
1.20
1.40
1.60
0 10 20 30 40
Temp (K)
EC
Series1
P. M. Grant
MgB2 – One Year Later
MgBMgB22: : JJcc at at 20K20K
ICSTM Centre for High Temperature Superconductivity
1.E+03
1.E+04
1.E+05
1.E+06
1 10B / Tesla
Jc A/cm2
virgin
Irrad.
ORNL thin film
Dresden bulk (nanoXtal)
Imperial bulk A
Imperial bulk B
USEFUL
USEFULATTAINABLE??
ATTAINABLE??
“B”
“A”
ORNL
P. M. Grant
MgB2 – One Year Later
Imperial Imperial CollegeCollege
MgBMgB2 2 progressprogress• Additive A (by scaleable route)
enhances Jc to levels comparable with micro-crystalline samples, and that that are useful for applications at 20Kare useful for applications at 20K.
• Additive B (by scaleable route) improves field dependence of Jc(B). NB, because of sample porosity, only a lower bound for magnitude of Jc.
P. M. Grant
MgB2 – One Year Later
Wire Actors• Institutions
– INFM-Genova– UniGe– Ames– IRL (NZ)– NIMS (Japan)
• Companies– HyperTech (USA)– Diboride Conductors (UK)– Pirelli (?)– AMSC (?)– IGC-SP (????)– Japan (?)
No HTS wire Companies presentlyHave “visible” MgB2
Development programsUnderway
P. M. Grant
MgB2 – One Year Later
Tape dimensions: 3.5 mm x 0.35 mmFilling factor 20%Treated at 900°C for 2 hours in Ar
INFM-Genova, G. Grasso, A. Malagoli, V. Braccini, S. Roncallo, and A.S. Siri, Italy
INFM-GenovaNi-Sheathed MgB2 Tape
Ex-Situ Sintered
0 2 4 6 8 10 121
10
100
1000
Htape
H//tape
I c at 4
.2 K
Magnetic Field [T]1.0x104 1.5x104 2.0x104 2.5x104 3.0x104
10
100
1000
Htape
Transport 4.2K
Cri
tica
l cu
rre
nt [
A]
Magnetic Field (Gauss)
Inductive 5K 10K 15K 20K 25K
4.2 K
4103
4104
4105
A/cm2
Asc = 2.510-3 cm2
P. M. Grant
MgB2 – One Year Later
Critical CurrentDensity, A/mm²
10
100
1,000
10,000
100,000
0 5 10 15 20 25 30
Applied Field, T
Nb3AlNb-Ti
2212
2223
At 4.2 K UnlessOtherwise Stated
2212
YBCO
MgB2
Film
YBCO75 K H||a-b
YBCO75 K H||c
1.8 K Nb-Ti-Ta
PbSnMo6S8
1.8 K Nb-Ti
Nb3Sn Tape from (Nb,Ta)6Sn5
Nb-TiHT
Nb-TiAPC
Nb3SnBronze Low Field
Nb3SnBronze High Field
Nb3SnHigh Sn
Critical CurrentDensity, A/mm²
10
100
1,000
10,000
100,000
0 5 10 15 20 25 30
Applied Field, T
Nb3AlNb-Ti
2212
2223
At 4.2 K UnlessOtherwise Stated
2212
YBCO
MgB2
Film
YBCO75 K H||a-b
YBCO75 K H||c
1.8 K Nb-Ti-Ta
PbSnMo6S8
1.8 K Nb-Ti
Nb3Sn Tape from (Nb,Ta)6Sn5
Nb-TiHT
Nb-TiAPC
Nb3SnBronze Low Field
Nb3SnBronze High Field
Nb3SnHigh Sn
YBCO75 K H||a-b
YBCO75 K H||c
1.8 K Nb-Ti-Ta
PbSnMo6S8PbSnMo6S8
1.8 K Nb-Ti
Nb3Sn Tape from (Nb,Ta)6Sn5
Nb-TiHT
Nb-TiAPC
Nb3SnBronze Low Field
Nb3SnBronze High Field
Nb3SnHigh Sn
Peter Lee’s Cosmic Plot (UW/ASC)MA/cm2
10
1
0.1
0.01
0.001
Power Apps30 – 77 K
HEPGenoa25 K
P. M. Grant
MgB2 – One Year Later
HyperTechRepresentative JC’s
Temperature, K 4K 4K 4KField, T 0-0.2 1 3Jc -kA/mm2 7.5* 3* 0.2
Temperature, K 30K 30K Field, T 0-0.2 1 Jc -kA/mm2 0.32 0.1 (over 300 amps) (over 100 amps) * by extrapolation due to flux jump and lack of stabilization
A/cm2 750,000 300,000 20,000
A/cm2 32,000 10,000
P. M. Grant
MgB2 – One Year Later
HyperTech MgB2 Wire
60 meters, 1.2 mm Mono MgB2 CTFF Iron in Monel
Multi-filament
P. M. Grant
MgB2 – One Year Later
WireCost Issues
Merit Factor for Superconducting Wire:C/P = $/kAmp × meters
Wire C/P Cost Driver
NbTi (4.2 K, 2 T) 0.90Materials
(Nb)
Nb3Sn (4.2 K, 10 T) 10Materials
(Nb)
Bi-2223 (25 K, 1 T) 20 Materials (Ag)
Y-123 (25 K, 1 T) 4 Capital Plant
P. M. Grant
MgB2 – One Year Later
MgB2 Wire C/P
Assumptions/Givens:• JC = 100,000 A/cm2
• IC = 2000 A/wire (Area = 2 mm2)
• Non-Materials C/P = 0.11 $/kA•m (NbTi)
Alfa Aesar MgB2 Price Quote (10 kg)• 750 $/kg (0.75 $/gm)
MgB2 Wire C/P• 2.03 $/kA•m @ 25 K, 1 T
P. M. Grant
MgB2 – One Year Later
Critical Wire Issues
20 – 30 K1 – 3 T
JC, Hirr Length
BSCCO/OPIT
YBCO CC
MgB2 ac Losses ?
++++ ++++
++++++
++++++++++
P. M. Grant
MgB2 – One Year Later
MgB2 Opportunities
20 – 30 K, 0 – 3 T
• Transformers
• Rotating Machinery
• Cables (?)
P. M. Grant
MgB2 – One Year Later
P.M. Grant, The Industrial Physicist, Feb/March Issue, 2002
ftp://ftpuser:[email protected]/outgoing/pgrant/SuperCity
SupermarketSchool Home
Family Car
DNA-to-order.com
Nuclearplant
H2
H2
MgB2
“SuperCity”