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Elvis Fornasiere | CERN, 26 th February 2013 TE-MSC-MDT Acknowledgments: G. Ambrosio, F. Cerutti, S....
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Transcript of Elvis Fornasiere | CERN, 26 th February 2013 TE-MSC-MDT Acknowledgments: G. Ambrosio, F. Cerutti, S....
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Acknowledgments: G. Ambrosio, F. Cerutti, S. Clément, L. S. Esposito, P. Ferracin, P. Fessia, R. Flukiger, R. Gauthier, M. Juchno, A. Mereghetti, N. Peray, J.-C. Perez, G. de Rijk, E. Todesco,
Radiation resistance of insulation systems for IR
Triplets
3
Outline
Outline
• Structural requirements for MQXF based on expected dose
• Measurement techniques for irradiated samples
• Experimental results on CTD-101K samples and CE-epoxy blend materials
• Experimental and FE simulations of the SBS Test on G10
• Suggested Plan
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
Plan
End
26 July 2012, joint WP2, WP3, and WP10 meeting
Beam screen shielding
Beam screen with W
absorbers at mid-planes
* 0.5 mm clearance between BP and W
4
Configurations Diameter aperture at mid-planes (mm)
3.7 mm BP + 7 mm W inserts 114.6
3.7 mm BP + 2 mm BS + 6 mm W absorbers* 111.6
Minimum aperture requested from optics is 116 mm
• To go below 20 MGy one would need 2 mm BS + 9 mm W absorbers(105.6 mm residual aperture)
• Maximum thickness shielding for Q1-first half Q2A tailor-made
• Possible use of other materials for BS/CB under investigation
With courtesy of F. Cerutti, L.S. Esposito on behalf of CERN FLUKA team [1]
140 mm Nb3Sn
Structural req + energy deposition
5
Q1 Energy deposition
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
With courtesy of F. Cerutti, L.S. Esposito on behalf of CERN FLUKA team [2]+[3]
Azimuthal energy deposition at Q1 peak
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
Plan
End
6 Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
t
tt
t
t
tt
t
30-40 MPa sheart
t t
t
Cool-down Max-gradient (155 T/m)
150 mm Nb3Sn Shear stress
50-60 MPa shear singularity?
Observation of Shear stress
between turns and shear between inner
and outer layers
~0 MPa shearWith courtesy of M. Juchno and P. Ferracin [4]
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
Plan
End
7 Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
With courtesy of M. Juchno and P. Ferracin [4]
150 mm Nb3Sn Azimuthal stress
Cool-down Max-gradient (155 T/m)
160 MPa compression stress
Risk of tensile stre
ss
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
Plan
End
8
Detailed coil model status
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
• “Rectangular” cable with 150um G10 insulation
• Cable material have similar properties as initial coil block (altered to spring model)
• High shear stress peaks at cable corners due to difference in thermal contraction
• Shear stress in coils up to ~30-40 MPa (cables and insulation around conductor in the vicinity of poles and copper blocks
• Possible next step: round “corners” or strand model with resin
With courtesy of M. Juchno and P. Ferracin [4]
Plan
End
9
Measurement techniques 1
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Test Nb 1 2 3 4
Name Flexural test Ultimate Tensile Test (UTS)
Mode I: intralaminar crack opening
Mode II: intralaminar shear mode
Diagram
Remarks Recommended by IEC. Most radiation-sensitive property for thermoset. Done at CERN for yellow books.
Tests used for radiation effects on insulators for superconducting fusion magnets by the ATI, Vienna. In order to load the anisotropic FRPs in mode I as well as in mode II under their weakest condition, the fiber orientation with the lower fiber content was chosen to be perpendicular to the notches of the specimens.
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
Plan
End
10
Measurement techniques 2
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Test Nb 5 6 7
Name Short Beam Shear (SBS). Interlaminar
Shear/compression test
10° off-axis tensile test
Diagram
Remarks SBS: interlaminar strength.
Other tests were done: double-lap-shear (DLS) test method, cycling test, etc. (not presented here).10° off-axis tensile test is normally used for intralaminar shear strength
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
Plan
End
11
ATI Vienna Facility 1
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
MTS 810 test facility
10 cm
5 cm
Short-beam-shear test
23 mm 6.4 – 6.5 mm
• Sample thickness should be 3 mm, preferably 4 mm. • At least 10 samples are needed for one test. • In case of a wrapped insulation, the tests should be
carried out parallel and perpendicular to the winding direction (10 + 10 samples).
• Approximately 90 shear samples can be irradiated in one run.
With the courtesy of R. Prokopec [32]
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
Plan
End
12
ATI Vienna Facility 2
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
• At least 5 samples are needed for static tests and additional 20 samples for stress lifetime curves.
• 20 samples can be irradiated in one run (for 4 mm sample thickness).
ATI d-ASTM
ASTM
Static: with and without strain recording
Dynamic: load controlled
Tensile tests
2010
140
70
10
Tensile test specimen geometries
With the courtesy of R. Prokopec [32]
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
• Dose rate: 40 MGy in 5 open days• 1 Container = 1 dose level• Costs: 50 MGy = 16 k€ per container + staff
Plan
End
13
Relative mechanical properties for CTD-101K
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
0 0 3 30 3001%
10%
100%
CTD-101K, with 50% Vf virgin S-2 Glass
Torsional Shear ModulusCompressive StrengthCompressive ModulusFlexural ModulusTorsional Shear StrengthFracture Resistance GICTorsional Shear StrainShear Strength
Absorbed dose (MGy)
Rel
ativ
e m
echa
nica
l pro
pert
ies
(tes
ts 7
7 K
) ILSS0 ≈ 120 MPa 30% degradation at 50 MGy
Shear strength and degradation with
irradiation is the most sensitive property
[29]+[30]+[31]
UTS: 35% reduction at 180 Mgy from UTS0 ~ 1050 MPaCompressive strength = 1080 MPa at 160 Mgy (Loss 20%)Fracture Resistance GIC: 66% reduction at 230 MGy
G10 SBS Test
70% degradation at 90 MGy
Plan
End
SBS test gives «apparent ILSS»
95% degradation at 160 MGy
14
Shear/compressive properties of CTD-101K
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
• Shear/compression failure envelope• Shear strength increases with
angle till 84°, then drops• Compression prevents shear
failure• On vertical plane (at peak dose
location), compression is huge and shear stress is small Almost pure compression state
0 200 400 600 800 1000 1200 1400 16000
50
100
150
200
250
300
Shear/compression failure envelope for CTD-101K virgin fibers insulation system at 76 K
0° (SBS)15°45°75°84°90° (compression)
Compressive Stress (MPa)
Shea
r Str
engt
h (M
Pa)
Angle
• 45° shear/compression test to characterize both types of heat treatment (14% reduction)
• No significant difference in mechanical properties between for specimen with and without heat treatment
• Not possible to compare interlaminar shear properties after 700°C heat treatment using SBS test (tensile mode failure) UTS of fibers significantly damaged
G10 SBS Test
[29]+[30]+[31]+[37]+[38]+[39]
Plan
End
FE studies on Shear/Compression test
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
15
• Comparison analytical vs numerical investigations shows inhomogeneous and tri-axial stress state.
• Considerable thermal stresses arise from cooling to cryogenic temperatures (not evaluated by analytical considerations)
• Failure of the specimens mainly takes place at the interface (influence of thermal stresses)
• The reliability of the test method is questionable if the specimen fractures at the interface. Strong dependency of surface conditions (arbitrary circumstances)
• Irradiation problem: high activation of steel plates
[37]+[41]
Plan
End
16
Mechanical properties for CE-epoxy blend
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
O
O
CH3
H
CN
C
N
Cyanate ester
(AroCy-L10)
G10 SBS Test
[32+[33]+[34]
Plan
End
G10 SBS experimental results
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
SBS [MPa] FSBS_1 FSBS_2 FSBS_3 FSBS_4 FSBS_5 Average Standard deviation Coefficient of variation %Series A 54.80 58.03 55.87 55.37 56.77 56.17 1.27 2.26Series B 53.50 54.22 52.14 48.32 51.68 51.97 2.28 4.39Series C 38.17 36.30 35.84 36.11 33.54 35.99 1.65 4.59Series D 54.91 56.28 55.86 55.04 54.86 55.39 0.64 1.16
Nb of
specimenL
(mm)b
(mm)t
(mm)l
(mm) l/t
Specimens A 5 24 10 4 12 3
Specimens B 5 24 10 4 16 4
Specimens C 5 42 10 4 28 7
Specimens D 5 24 6 4 16 4
With the courtesy of A. Gerardin (EDMS N° 1259235) + [40]
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
17
Plan
End
FE studies on SBS test
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
18
• f-factor = 1 inside the specimens the stress is equal to the shear stress obtained from an analytical 2D solution
• The real “ILSSs” are higher than the experimental results
[36]
Plan
End
G10 SBS FE results
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
19
Shear at D (MPa) Shear at F (MPa)Sigma x at F Inside (MPa)
Sigma z at F Inside (MPa)Exp. ILSS SBS
(MPa) Inside Outside f-factor Inside Outside
Series A 56.17 55.61 67.97 1.22 129.79 140.24 374.48 -127.01
Series B 51.97 51.05 63.63 1.25 125.01 130.38 454.98 -122.71
Series C 35.99 33.99 43.84 1.29 88.36 82.41 509.98 -86.82
Series D 55.39 55.38 64.83 1.17 133.19 147.61 494.08 -130.83
Contrainte de rupture à la flexion, <= 10 mm perpendiculairement aux strates, sens longitudinal : > 350 N/mm2
Plan
End
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
20
21
Suggested planInternal test campaign prior to irradiation campaign (unirradiated fibers)• SBS test of heat treated fibers with 3 resins (CTD-101K,
CE/epoxy blend, MY750)• Resin with 1)virgin fiber, 2) 50h @700°C fiber, 3) 50h @700°C ht fiber +
ceramic binder + 4) 50h @700°C ht fiber + PVA
• 10° off axis-test as support of SBS test• Shear/compression test of the system [cable + insulation]
Irradiation campaign (to be discussed)• What is the maximum dose level (20 MGy)?• SBS – Interlaminar shear test (qualitative)• Shear/compression test of the system [cable + insulation]
(Quantitative)
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
CTD-101K MY750 CE
Virgin fibers
Fibers after reaction
Fibers after reaction and ceramic binder
SBS + Tensile +/- 10° +
shear/compression
Plan
End
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
22
Thanks for your attention
Questions?
Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
Plan
End
Outline
Structural req + energy deposition
Measurement techniques
CTD-101K + CE-epoxy
results
G10 SBS Test
24 Elvis Fornasiere | CERN, 26th February 2013 TE-MSC-MDT
With courtesy of M. Juchno and P. Ferracin [4]
150 mm Nb3Sn Radial stress
References1. F. Cerutti, L.S. Esposito on behalf of CERN Fluka team, “Shielding the 140 option”, Hi-Lumi LHC WP10, CERN, 26
July 2012.2. F. Cerutti, L.S. Esposito on behalf of CERN Fluka team, “First estimates of energy deposition for the new inner
triplet”, Hi-Lumi LHC WP10, CERN, 7 June 2012.3. L.S. Esposito, private communication, CERN, 25.02.2013.4. M. Juchno, private communication, CERN, 25.02.2013.5. C. Barrère, D. Dal Maso, Résines époxy réticulées par des polyamines: structure et propriétés, Revue de L’Institut
Français du Pétrole, Vol. 52, N° 3, Mai-Juin 19976. P. Bardonnet, Résines époxydes (EP) – Composants et propriétés, Doc. A 3 465, Techniques de l’Ingénieur, 20127. T. Devanne, Vieillissement radiochimique d’un réseau époxyde, Thèse N° 2003-05, E.N.S.A.M, 16 Mai 20038. D.W. Clegg, A. A. Collyer, Irradiation effects on polymers, Elsevier Science Publishers LTD, London, 19919. A. Idesaki, A. Shimada, N. Morishita, M. Sugimoto, M. Yoshikawa, Evalutation of Radiation Resistance for
Organic Materials Used in Atomic Energy-related Facilities, Radiation Effects in Super Conducting Magnet Materials (RESMM’12), Fermilab, February 13-15,2012
10. D. Reed, Radiation Tolerance of Resins, Rad-Hard Insulation Workshop, Fermilab, April 20, 200711. H. Schönbacher, A. Stolarz-Izycka, Compilation of radiation damage test data – Part II: Thermosetting and
thermoplastic resins, CERN 79-08, Geneva, 197912. M. H. Van de Voorde, Effects of radiation on materials and components, CERN 70-5, Geneva, 197013. M. H. Van de Voorde, Action des radiations ionisantes sur les résines époxydes, CERN 70-10, Geneva, 197014. M. Tavlet, A. Fontaine and H. Schönbacher, “Compilation of radiation damage test data, pt.2: Thermoset and
thermoplastic resins, composite materials”, CERN-98-01, Geneva : CERN, 1998. - 173 p.
2526/02/2013 E. Fornasiere
References15. International Electrotechnical Commission, Geneva, Publication No. 544: Guide for determining the effects of
ionizing radiation on insulating materials, Part I: Radiation interaction, Ref. 544–1 (1977); Part 2: Procedures for irradiation, Ref. 544–2 (1979); Part 3: Test procedures for permanent effects, Ref. 544–3 (1979); Part 4: Classification system for service in radiation environments, Ref. 544–4 (1985).
16. D.C. Phillips et al., The selection and properties of epoxide resins used for the insulation of magnet systems in radiation enviroments, CERN 81–05 (1981).
17. H. Schönbacher, B. Szeless and M. Tavlet, “Results of radiation tests at cryogenic temperature on some selected organic materials for the LHC”, CERN 96-05, Geneva, 1996
18. G. Lipták et al., “Radiation tests on selected electrical insulating materials for high-power and highvoltage application”, CERN 85–02, Geneva, 1985.
19. H. W. Weber et al., “Low temperature neutron and gamma irradiation of glass fiber reinforced epoxies”, Journal of Nuclear Materials 115 (1983) 11-15
20. K. Humer et al., “Radiation effects on insulators for superconducting fusion magnets”, Cryogenics 35 (1995) 871-882
21. René Flükiger, Gijs de Rijk, “Review of WAMSDO 2011 Workshop: Superconductors in LHC Upgrade (HiLumi LHC)”, RESMM’12, Fermilab, 13-15.02.2012
22. Ezio Todesco, “ High Luminosity LHC: Magnets”, Applied Superconductivity Conference, Portland, 9th October 2012
23. P. Ferracin, “MQXF coil cross-section status”, HiLumi WP3 Video-meeting, 28 August, 201224. P. Fessia, “The CERN magnet program and the conductor needs”, LTHFS Worhshop, Napa Valley – 5th to 7th
November 2012
2625/02/2013 E. Fornasiere
References25. K. Humer et al., “Tensile and shear fracture behavior of fiber reinforced plastics at 77 K irradiated by various
radiation sources”, Adv. Cryog. Eng. 40 (1993)26. K. Humer et al., “Low temperature tensile and fracture mechanical strength in mode I and mode II of fiber
reinforced plastics following various irradiation conditions”, Fusion Technology 199427. K. Humer et al., “Tensile and fracture behavior in mode I and mode II of fiber reinforced plastics following
reactor irradiation”, Advances in Cryogenic Engineering (1996), Vol. 4228. K. Humer et al., “Low-temperature interlaminar shear strength of reactor irradiated glass-fibre-reinforced
laminates”, Cryogenics 36 (1996) 611-617 29. Composite Technology Development, Inc. “CTD-101 and CTD-101K Epoxy Resin System”, Datasheet, 2003.30. Composite Technology Development, Inc. “CTD-101K Epoxy Resin System”, Datasheet, 2003.31. Composite Technology Development, Inc. “CTD-101K Epoxy Resin System”, Datasheet, 2012.32. N. A. Munshi, J. K. Walsh, M. W. Hooker, H. K. Babcock, “Radiation Resistant Electrical Insulation Qualified for
ITER TF Coils”, Applied Supeconductivity Conference, Portland (OR), October 2012.33. Composite Technology Development, Inc. “CTD-400 Series Cyanate Ester Resins for RTM High Performance,
Eady Processing”, Datasheet, 2002.34. Composite Technology Development, Inc. “Cyanate Ester-based Insulations Summary Data Sheet”, Datasheet.35. R. Prokopec, “Mechanical tests on radiation resistant insulation materials”, PPT Presentation, 19.12.201236. D.H. Pahr, F.G. Rammerstorfer, P. Rosenkranz, K. Humer, H.W. Weber, “A study of short-beam-shear and double-
lap-shear specimens of glass fabric/epoxy composites”, Composites: Part B 33 (2002) 125-132.37. D.H. Pahr, H.J. Böhm, K. Humer, H. W. Weber, “Analytical and finite element investigations of shear/compression
test fixtures”, Cryogenics 45 (2005), 606-616.
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References38. P.E. Fabian, J. B. Schutz, C. S. Hazelton, R. P. Reed, “Properties of candidate ITER Vacuum Impregnation
Insulation Systems”, Advances in Cryogenic Engineering, Vol. 40, New York, 199439. P.E. Fabian, R.P. Reed, J.B. Schutz, T.S. Bauer-McDaniel, “Shear/compressive properties of candidate ITER
inuslation systems at low temperatures”, Cryogenics 35 (1995) 689-69240. R. P. Reed, J. B. Darr, J. B. Schutz, “Short-Beam Shear Testing of candidate magnet inulators”, Cryogenics (1992),
Vol. 32 ICMC Supplement41. H. Weber, private communication, Email exchange, 19.02.2013.
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