aaron aoyama 1, j. blanchard 2, n. ghoniem 1, s. sharafat 1* 1 university of california los angeles...
TRANSCRIPT
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Aaron Aoyama1, J. Blanchard2, N. Ghoniem1, S. Sharafat1*
1University of California Los Angeles2University of Wisconsin Madison
With Contributions FromJ. Sethian3, S. Abel-Khalik4, A. Robson3, F. Hegeler3,
M. Wolford3, and J. Parish5
3Naval Research Laboratory4Georgia Institute of Technology
5Commonwealth Technology, Inc6Oak Ridge National Laboratory
1
18th High Average Power Laser WorkshopHosted by Los Alamos National Laboratory
Hilton Santa Fe Historical Plaza100 Sandoval Street, Santa Fe, New Mexico, USA
April 8-9, 2008
Thermo-Structural Analysis of the HIBACHI-Foil
*[email protected] This work was supported by the US Navy/Naval Research Laboratories through a grant with UCLA.
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OUTLINE
• Geometry and Loads• Exp. Performance Statistics• Thermo-Structural Analysis• Summary
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Hibachi Foil Geometry
100 cm
30 cmFoil
Water cooledSupport Ribs Vacuum Side
Commonwealth Technology, Inc.J. Parish – 2008
Foil: 304 SS; 25 m thick
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LoadingTemperatures:
Tfoil ≈ 180 oC – 450 oCTfoil ≈ 30 oC (swing/shot)
Laser Gas Pressure:P ≈ 20 psi (0.138 MPa)
Load Duration:f = 5 Hztheat ≈ 140 ns (heating)tmech≈ 10 s (mechanical)
J. Sethian et al., NRL 2008
Hibachi Configuration
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Global Performance StatisticsFor runs: 5/13/04 to 1/16/08• 447,963 shots• 63 different foils• 33 foil failures
• 18 failures due to holes• 15 failures due to “blows”• Max : ~25,000 shots (no wrinkles)
Total Foil Lifetime Classified by Heat Wrinkles
0
1
2
3
0 5,000 10,000 15,000 20,000 25,000 30,000
Total Number of Shots
Wrinkle
No Wrinkle
Unknown
J. Se
thia
n et
al.,
NRL
200
8
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Global Performance StatisticsFoil Failure Classified by Mode and Wrinkle
Wrinkle, 6
Wrinkle, 4
No Wrinkle, 9No Wrinkle, 10
Unknown, 3
Unknown, 10
2
4
6
8
10
12
Hole Blown
Num
ber
of r
uns
J. Sethian et al., NRL 2008
Hole Blown
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Thermo-Structural AnalysisFour Models:(1)Flat foil(2)Curved foil(3)Flat foil+ Curved Rib(4)Scalloped
Analysis• Shell Elements• Pressure Load• Pressure +Thermal• Linear/Non-linear
Foil stress-strain measurements...Electra Hibachi vs the professionals
0
10
20
30
40
50
60
70
0 0.005 0.01 0.015 0.02 0.025 0.03strain
stress(ksi)
Foil Strip: B31590
Foil Strip: G47536
Electra 12/ 27/ 07
Electra 01/ 09/ 08
414
276
138
MPa
345
207
69
J Parish, CTI Inc. 2008
Properties:Temperature 20 oC 400 oCYoung's Modulus 200 GPa 170 GPaTangential Modulus 1.8 Gpa 1.8 GPaYield Strength 310 MPa 207 MPa
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3.4 cm
30 c
m
With all four outer edges fixed, and pressure applied, the model deforms plastically.
5 Cycles at 400 oC:Stress ~ 340 MPaStrain ~ 3.9 %(max along rib edges)
(1) Flat Model: Pressure Only Stress Contours
Yield~207MPa at 400 oC
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Stress Displacement Strain
max ~ 340 MPa dmax~3 mm wrinkle~0.05
Model 1: Flat Foil – Pressure & Temp.After pressurizing heat is applied
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Flat Model: Pressure & TemperatureStressDisplacement Strain
max~340MPadmax~3 mm wrinkle~0.05
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Model 2: Curved Foil Before Loading
To further examine the high strains along edges, a surface with curvature (only along the width) was modeled under the same loading conditions.
7 mm
Cross-section view
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Pressure Loading
With all four edges fixed, and pressure applied, the model deforms elastically.
Pressure & TemperatureIn this case, the “wrinkle” caused by thermal expansion is very localized.
Is the foil buckling?
Plastic strain contours
Displacement (magnitude) contours
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Nonlinear Buckling Analysis
A more conservative approach is to use a nonlinear buckling analysis.
In this case, the temperature load is increased until the solution begins to diverge.
Then, an ANSYS nonlinear stabilization option adds an artificial damper to maintain a stable state.
The damping coefficients are tracked and are used to make corrections to the results. Displacement (magnitude) contours
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Plastic Strain Contours
Von Mises Stress Contours
Model 2: Curved Foil Non-linear Buckling
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This analysis examined the effects of curving the supports that hold the foil in place.
This is done to attempt to alleviate the very large rotations of the foil about the long edges.
Model 3: Flat Foil, Curved Support
Front View
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It is immediately apparent that the shape of these rigid supports ease the transition to the foil’s equilibrium state.
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Compared to the original flat model (Case 1) with a similar mesh density, there is a significant decrease in plastic strain.
Original Flat Foil
With Curved Supports
Max Plastic Strain: 0.039
Max Plastic Strain: 0.016
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This analysis examined the effects of curving the supports and curving the foil.
This is done to attempt to further alleviate the rotations of the foil about the long edges.
Model 4: Scalloped Foil Scalloped Foil Test Section
J Parish, CTI Inc. 2008Details of the Scallops
(inches) [mm]
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This non-linear analysis assumes the foil can slidealong the curved rib(analyze small section with symmetry BC, 1064 elements)
Effects of foil end geometry is absent.
Model 4: Scalloped Foil – Pressure
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Displacement Contours
At max. pressure: 26.6 psi
Factor 100 smaller from flat modelFactor 70 smaller from flat with curved ribs
Foil slides on curved structure(graphical artifact of thin shell element s)
The shape of these rounded supports and rounded foil ease the transition to the foil’s equilibrium state resulting in small deformations 30 m
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Stress Contours
At max. pressure: 26.6 psi
Foil slides on curved structure(graphical artifact of thin shell element s)
Max. stress 170 MPa along the edge (below yield)Foil stress fairly uniform
With this geometry , and only pressure applied, the foil deforms elastically.
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Strain Contours
At max. pressure: 26.6 psi
Foil slides on curved structure(graphical artifact of thin shell element s)
Max Plastic Strain 0.0005 along the edge
Significantly smaller from flat foil: 100 less 50 less from curved foil & flat foil with curved structure
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Residual Stress: Unload from 26.6 psi to 0 psi
Residual stress levels arelow: 0.065 MPa (pressure only)
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Summary• Four Models were investigated:
(1) Flat foil(2) Curved foil(3) Flat foil & curved support(4) Scalloped foil– Pressure + Thermal loads of (1) shows wrinkle formation– Pressure + Thermal load of (2) inconclusive (pressure alone shows ½
strain of flat; wrinkles using non-linear buckling)– Pressure (only) of (3) shows ½ strain of flat – Pressure (only) analysis for Scalloped (4) shows:
• Max. Displacement factor of 100 less than (1)• Max. Stress factor of 2 less than (1)• Max. Plastic strain ~100 X less than (1) and 40 X less than (2) & (3)
• Effects of thermal load and “end-geometry” for scalloped foil remains to be analyzed
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Additional Slides
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Buckling Analysis
An conservative eigenvalue buckling analysis was performed to determine an approximate first buckling mode.
From this preliminary analysis, it appears that under temperature loading, when the foil buckles, the largest deflections are near the ends.
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x
yX-Component Plastic Strain
Y-Component Plastic Strain
εx,max = 0.013
εy,max = 0.012
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Nonlinear Contact Analysis
Foil Mesh• SHELL181 (4 node quad): shell elements that
support large displacements, membrane stresses, and account for change in shell thickness
• CONTA174: contact surface elements
Support Mesh• TARGE170: rigid target surface elements
Loading • 3-edge fixed• Modeled one side – 1 symmetry B.C.• Pressurized
Solution• Adjusts small gap to bring surface to initial
contact• Solved for 4000 and 16000 nodes
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Mechanical AnalysisMechanical Analysis
Sharafat-UCLA
Made a six-rib section of the Hibachi foil Used shell elements for elastic and plastic analysis Estimated Young’s Modulus (E) and Tangent Modulus (Etan) based on NRL Data.
Test Temp. & Condition E (GPa) Etan (GPa) Yield (MPa)NRL Data
21 oC as received 39.16 2.26 31021 oC exposed 36.82 1.27 434400 oC as received 12.59 3.29 209400 oC exposed 17.22 8.41 365
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Pressure LoadsPressure Loads
Sharafat-UCLA
Analyzed 5 pressure pulses ( 6.5 psi)
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Stress for 5 Pulses (400 C exposed)
Sharafat-UCLA
Residual stress following first pulse: 0.47 MPa
Pulse Residual Stress* (MPa)
1 0.47
2 0.30
3 0.20
4 0.30
5 0.30
*assumes constant material properties
Node 15129 (max stress)