review on stress sensitivity part i
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Review on stress sensitivity Part I. R. Flükiger B. Seeber Group of Applied Physics (GAP) University of Geneva. Outline General problematics of stresses in superconductors ITER and NED requirements Uniaxial tensile stresses: J c vs. e Models for description - PowerPoint PPT PresentationTRANSCRIPT
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Stress review - CERN, 4.11.2008
Review on stress sensitivity Part I
R. FlükigerB. Seeber
Group of Applied Physics (GAP)
University of Geneva
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Outline
General problematics of stresses in superconductors
ITER and NED requirements
Uniaxial tensile stresses: Jc vs.
Models for description
Transverse compressive stresses: Jc vs. t
What do we actually know?
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Requirement for ITER ≠ Requirement for NED
Requirements for Jc and stresses:
ITER: Jc(non Cu) > 1’100 A/cm2 at 12 T
low a.c. losses filament diameter < 20 mm
No impregnation, no particular mechanical protection
No cracks up to 30 MPa: twist pitch/bending
Direct contact between strands: transverse stresses !!!
No relevant degradation of Jc after > 20 years (neutrons)
NED: Jc(non Cu) ≥ 1’500 A/cm2 at 15 T
No cracks up to 120 MPa
Impregnation, reduces problems of transverse stresses
No relevant degradation of Jc after 10 years (neutrons)
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The ITER TF Model Coil
ø 40 mm, 1.5 mm thick steel
Conduit rated current:
70 kA/11.8 T/4,6 K
1028 strands
Nb3Sn + 1/3 Cu
Nb3Sn Conductor
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Internal Sn Diffusion Technique
Example: Oxford Instruments, for ITER Type I)
* 0.81 mm (NbTi)3Sn strand * 19 subelements *) * Single Ta barrier * Cu:non-Cu ratio 1 * Jc ~1200 A/mm2 (Type I) ~1100 A/mm2 (Type II) * Non-Cu hysteresis losses: 900 kJ/m3 (Type I) 700 kJ/m3 (Type II) * Unit lengths: up to 8 km
*) Agglomeration of original filaments during reaction: Characteristics of Internal Sn wires
Courtesy A. Vostner, ITER5
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Problem: All high field superconductors are brittle. At fracture ≤ 0.05 %: Formation of cracks
Only exception: NbTi, with Tc = 10K, Bc2(0) = 14 T
Question: How can one built large magnets based on superconducting wires with
irr ≥ 0.6% ?
Answer: Microfilamentization Reason: Relationship between contact surface and volume (or: Ratio between Interface and total filament surface)
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Microfilaments
Bronze Route wire 100 nm
2 m 7
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wire name wire N. of filaments
Fil. eff. diameter
A15 layer thickness
Cu A15 volume fraction
GAP#14-#24 Ti, Ta 1.25 mm 14641 4-5 m 2-3 m 20% 23%2%
OST #7069 Ti 0.8 mm 18 70 m 10-30 m 59% 23.5%1%
OST #8056 Ti, Ta 0.9 mm 60 100 m 20-25 m 30% 42%2%
OST #8298 Ta 0.9 mm 60 100 m 20-25 m 30% 38%2%
SMI Ta 1 mm 192 50 m 10 m 45% 25%0.5%
BronzeInternal Sn
PIT
4-5 m
70 m
70 m
50 m
Internal Sn wire PIT wire
Filament size D: D(bronze) << D(Internal Sn, PIT)irr(bronze) > irr(Internal Sn, PIT) > 0.8 % ≤ 0.4 %
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10 m
24 h/800°C
1 m
24h/850 °C
Main Limitation: above 560°C, the submicron size filaments are interrupted, due to the formation of Nb3Sn : “Spherodization”
10 m 1 m
The unfulfilled dream of Nb3Sn wires: « in situ » wires, with filament sizes < 100 nm
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Strengthening of « In Situ » wires (effect submicron filaments)
Increase from 0.3 to 0.7 %
Dendrite sizes after casting
Final wire: Sizes < 100 nm
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« in situ » techniquegiven upJc too low
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Tensile stresses
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650°C 4.2 K
Cu
Cu/Sn
Nb
Nb3Sn
cool down
m
•Cu and Cu/Sn in extension
•Nb and Nb3Sn in compression
Nb3Sn technical wires
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Origin of precompression in superconducting wires
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-1.5 -1.0 -0.5 0.0 0.5105
106
107
108
109
Eng
inee
ring
Crit
ical
Cur
rent
Den
sity
(A
m-2)
0.1
1
10
100
1000
Temperature: 4.2 K
Crit
ical
Cur
ren
t (A
)
23 T
Magnetic Field: 8 T
Applied Strain (%)
Nb3Sn Wire
Why is the effect of tensile strain important?
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Change of physical properties when applying a tensile stress
In Nb3Sn, the application of tensile stress has been recognized to change primarily the phonon spectrum rather than the electronic density of states(Markiewicz 2005, Hampshire et al., 2006)
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Tc/Tcm
Asymmetric behavior of Bc2()
Bc2()Bc2m
Effect of tensile stress much stronger on Bc2 than on Tc
Bc2()/Bc2m = 1 – a|o|
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10% reduction of Tc/Tcm: m: - 0.89%10% reduction of Bc2()/Bc2m: m: - 0.45%
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Elastic tetragonal distortion under the effect of uniaxial tensile stress
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GAP (Nb,Ti)3Nb - #14GAP (Nb,Ta,Ti)3Sn- #14
Uniaxial strain behavior of Nb3Sn wires
Internal Sn wires (Type I) are more strain sensitive than Bonze Route Wires. Asymmetry of Jc() observed for all wire types. Explanation by asymmetric distortion at both sides of m.
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q
c
p
cc B
B
B
BBJ
2
1
2 1),(
SBB cc 022
7.11)( maS
0
20
2
1
1)(
a
ma
C
CS
Ekin model ten Haken model
Kramer’s law
Field and strain scaling laws for Nb3Sn
strain dependent critical field
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-0.4 -0.3 -0.2 -0.1 0.0 0.1 0.20.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
21T, 4.2KB
c2=25T
intrinsic strain (%)
Ic/Ic
m
-0.4 -0.3 -0.2 -0.1 0.0 0.1 0.20.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
0=
0.25
0.15
0.08
0.02
Ca=
303540
50
intrinsic strain (%)
Ic/Ic
m-0.4 -0.3 -0.2 -0.1 0.0 0.1 0.2 0.3 0.4
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
a=900110013001500
21T, 4.2KB
c2=25T
B = 21 T
intrinsic strain (%)
Ic/Ic
m
Ekin’s model
ten Haken’s model
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Devices for Tensile Stress Measurements
Principle: Gradual release of the precompression
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a: The Pacman strain device (University of Twente)
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b) The Walters Spiral (Univ. Geneva)
•Max current 1’000 A
•Wire length up to 1 meter
•Max voltage tap distance 50
cm
•Jc criterion 0.01V/cm
Measurements: up to 21 T
Strain e: applied by an axial rotation
see: B. Seeber (next speaker)
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Steel reinforced Nb3Sn wires
Stainless Steel 316LN leads to a higher precompression
* higher non-hydrostatic tetragonal deformation
* higher hydrostatic compression
Depending on the Steel:Nb3Sn ratio, em increases from 0.25 to 0.87%
For 40% steel, a decreases of Bc2 by 3 T is observed
Lower Jc values are measured: for em = 0.87%, Jc/Jco = 0.12.
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Steel reinforced Nb3Sn wires
J.Ekin, W.Specking, R.Flükiger, J.Appl. Physics, 54(1983)2869
Fe/Nb3Sn
Jc/Jco
Stainless steel
Cu
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Transverse compressive stresses
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Fixed part
Moving part
Specifications:
- F = 5KN- I = 1000 A- Field 21 T
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0 100 200 300 400 500
t
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Conclusions
•Jc(B,) have been measured at very high fields (21 T) for Nb3Sn Bronze Route, Internal Sn and PIT wires.
•The results show a dominant effect of the axial components 1 D approximation: Jc(B,) curves usually analysed with the Ekin and ten Haken models
•3D distribution revealed by crystallography. Calculations still needed for larger filament sizes (subelements)
• Transverse compressive stresses: still no theoretical understanding. The very low reversibility of Jc suggests that nano- and microcracks are the major responsible for the much observed effects, which are much stronger than for uniaxial tensile stresses.
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