kdemo structural analysis p. titus june 26 2013. ! kdemo coil axisymmetric analysis pfcb 21 1,...
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KDEMO Structural Analysis P. Titus June 26 2013
! KDEMO coil axisymmetric analysispfcb211, 1.52,0.70,.9,1.3,8,10 !CS12, 1.52,2.10,.9,1.3,8,10 !CS23, 1.52,3.50,.9,1.3,8,10 !CS34, 1.52,4.90,.9,1.3,8,10 !CS45, 2.98,8.31,.60,1.25,8,10 !PF16, 3.66,8.31,.60,1.25,8,10 !PF27, 4.34,8.59,.60,1.25,8,10 !PF38, 5.02,8.75,.60,1.25,8,10 !PF49, 12.96,7.50,.849,1.5 ,8,10 !PF510, 14.88,2.95,.4,.5 ,8,10 !PF611, 14.88,-2.95,.4,.5,8,10 !PF612, 12.96,-7.50,.849,1.5,8,10 !PF513, 5.02,-8.75,.60,1.25,8,10 !PF414, 4.34,-8.59,.60,1.25,8,10 !PF315, 3.66,-8.31,.60,1.25,8,10 !PF216, 2.98,-8.31,.60,1.25,8,10 !PF117, 1.52,-4.90,.9,1.3,8,10 !CS418, 1.52,-3.50,.9,1.3,8,10 !CS319, 1.52,-2.10,.9,1.3,8,10 !CS2L20, 1.52,-0.70,.9,1.3,8,10 !CS1L21, 6.1,0,2.1,4.2,8,10 !Plasma
pfcu21,3,1,1.01,7.68,3.11,-1.552,7.68,3.11,-1.553,9.65,3.25,-2.254,9.65,3.25,-2.255,2.323,4.506,5.7156,3.171,6.235,7.9097,3.475,6.169,7.8978,3.663,5.286,6.9149,0.021,-13.70,-15.9510,0.184,0.135,-0.22311,0.184,0.135,-0.22312,0.021,-13.70,-15.9513,3.663,5.286,6.91414,3.475,6.169,7.89715,3.171,6.235,7.90916,2.323,4.506,5.71517,9.65,3.25,-2.2518,9.65,3.25,-2.2519,7.68,3.11,-1.5520,7.68,3.11,-1.5521,0,13,13
KDEMO Poloidal Coil Analysis
Poloidal Field Vectors
Kdm1.dat
Kdm2.dat
Kdm3.datNot 11 Tesla
Nodal ForceVectors
Kdm1.dat
Kdm3.dat
Kdm3.dat
DEMO CS CICC Parameter (Corner Channel)• Cable Pattern: (2SC+1Cu)x3x4x4x6 [576 SC Strand + 288 Cu Strand]• Void Fraction : 35.85%• Strand :
– ITER Type (Jc ~ 1000A/mm2) Nb3Sn Strand– Cu/Non-Cu = 1.0
• NO COOLING SPIRAL Corner Channel• Jacket Thickness : 5 mm• Insulation : 2.0 mm (with Voltage Tap)
– 0.1 mm Kapton 400% – 0.4 mm S-glass 400%
• Twist Pitch– 1st Stage 20 ± 5 mm– 2nd Stage 45 ± 10 mm– 3rd Stage 85 ± 10 mm– 4th Stage 150 ± 15 mm– 5th Stage 355 ± 20 mm
• Wrapping Tape Thickness – Sub-cable : 0.08 mm 40%– Sub-cable wrap width : 15 mm– Cable : 0.5 mm 60% – Final wrap width : 7 mm
DEMO CS CICC Cross-section
54
34
20
40
R 32 5
50
30
Insulation
Jacket
Hoop Multiplier = 459/173.7 = 2.64
Initial MagnetizationKdm1.txt, kdem1.datBased on the hoop multiplier76.1*2.64 = 200 MPa
Starts at 662 then propagates into region that is about 200 MPa
ITER CS Conductor near Butt Weld ITER CS He Penetration
Starts at 356 then propagates into region that is about 325 MPa
Average Hoop Stress =5.327e7/1.17/1e6=45.5MPa
Initial Magnetization Check of Average Hoop Stress
Based on the CS hoop multiplierApplied to PF590.6*2.64 = 240 MPa
Based on the CS hoop multiplierApplied to PF5126*2.64 = 332 MPa
TF Case 2/3* yield = 666 MPa½ Ultimate = 750 Mpa1/3 Ultimate = 500 MPa
Sm, Primary Membrane Allowable = 666 MpaAccording to ITER MSDC
The average stress in the inner leg case should satisfy this Allowable
TF Case and Winding Pack Analysis
Meshed areas from Tom’s Parasolids
Initial Geometry Without Added Outer Structures
Base Cross Section, Reflected and Swept Along Tom’s Arcs
kdm1 Field Vectors
Nodal Force VectorsField Vectors
kdm1
Kdm1 Theta Displacement
Kdm1 Tresca Stress
TF Case 2/3* yield = 666 MPa½ Ultimate = 750 Mpa1/3 Ultimate = 500 MPa
Allowable = 666 MpaAccording to ITER MSDC
TF Case 2/3* yield = 666 MPa½ Ultimate = 750 Mpa1/3 Ultimate = 500 MPa
Allowable = 666 MpaAccording to ITER MSDC
Added Upper Structure
Adde
d O
uter
Str
uctu
re
Added Lower Structure
Model with 16 fold Symmetry, 12 fold symmetry Expansion
Model with Added Structure
TF Case 2/3* yield = 666 MPa½ Ultimate = 750 Mpa1/3 Ultimate = 500 MPa
Allowable = 666 MpaAccording to ITER MSDC
Results with Added Structure
Still Doesn’t Pass
From the NSTX structural criteria.
"An exception to this elastic analysis approach can be when the nature of the structure and its loading make it difficult to decompose the stresses into the above mentioned categories. In such an instance, a detailed, non-linear analysis that accounts for elastic-plastic behavior, frictional sliding and large displacement shall be used to determine the limit load on the structure. The limit load is that load which represents the onset of a failure to satisfy the Normal operating condition as described in Section I-2.6. The safety factor of limit load divided by the normal load shall be greater than 2.0.“
Similar wording is in the ITER Magnet Structural Design Criteria (MSDC)
Try Elastic-Plastic Limit Analysis.Must Show a factor of 2 on failure (Non-Convergence in ANSYS Model)
Results with Load Factor of 2.0
Plastic Strain at Twice Normal Loading
Un-Loaded Results After Twice the Normal Loads are Applied
Old 2D TF Cross Section
An approximation of the options suggested by Keeman Kim is analyzed. The model Inner leg has an inner radius of 2.0m and OR = 3.14m. The inner wedged section is .286 m thick.
This section can support the centering load but depending on the position of the outer leg and the stiffness/strength of the outer structures, the inner leg cross section could be acceptable. However with only 27% of the vertical separating force on the inner leg, the cross section is inadequate.
Limit analysis is used to evaluate the section. With only the centering load, the load factor is above 3. With 27% of the bursting force applied to the inner leg, the load factor goes to only 1.5. It should be at least 2.0.
Heavy/stronger, and stiffer outer structures are needed to support ,most of the vertical bursting load.
The Bursting Force – is Applied on the Inner Leg Cross Section at a Coupled Node Set.
In the runs with the bursting load, 200MN is applied of the 11946/16 = 750 MN per coil, or 27% – The remainder is assumed taken by the outer structures
16 Fold Symmetry Expansion
Model Materials
Conductor Stress Strain
316 SST Stress Strain
Bmax=13.13
ANSYS Nodal Forces
ANSYS Displacement Constraints
ANSYS CP’s on Top Face
Vertical Separating Force is Applied on One of the Coupled Nodes on the Top Face
Von Mises Stress 2.5*Load
Von Mises Plastic Strain 2.5*Load
Excluding Vertical Separating Force
/DSCALE,1,20(20 times actual)
Including Scaled 200MN Vertical Separating Force
/DSCALE,1,20(20 times actual)
Radial Displacement Under Increasing Load
Collapses at Step 7 > 3 times the Nominal Load
Including Scaled Vertical Separating Force
Excluding Scaled Vertical Separating Force
Radial Displacement Under Increasing Load
Collapses at Step 3 or 1.5 times the Nominal Load
Radial Displacement Under Increasing Load
Collapses at Step 7 > 3 times the Nominal Load
Plastic Strain in the Nose
Remains Elastic up to Load Step 4, 2.0Times the Nominal Load
Excluding Scaled Vertical Separating Force
Excluding Scaled Vertical Separating Force
Conductor Total StrainNormal Loading Including 200MN Vertical Separating Force
Radial Total Strain
Theta Total Strain Von Mises Total Strain
Axial Total Strain
Normal Loading Including 200MN Vertical Separating Force
Normal Loading Including 200MN Vertical Separating Force
Insulation Von Mises Stress