Title: Review of the Stress Analysis of the MiniBooNE Horn MH1
1Review of the Stress Analysis of the MiniBooNE
Horn MH1
- Larry Bartoszek, P.E.
- 1/20/00
- BARTOSZEK ENGINEERING
2Overview 1
- The MiniBooNE horn carries 170 kiloamps of
current in a pulse 143 microseconds long. - The pulse repeats 10 times in a row, 1/15 sec
between each pulse, then the horn is off until 2
seconds from the first pulse in train. - The horn is stressed by differential thermal
expansion and magnetic forces. We need to design
it to survive 200 million cycles with gt95
confidence.
3Overview 2
- Motivation for design lifetime
- The horn will eventually become very radioactive
and require a complicated handling procedure in
the event of a replacement. We dont want to
make many of these objects. - We cant afford to make many horns.
- The major design issue is fatigue.
- Every component around the horn needs to survive
200 million pulses to get overall system
reliability.
4Analysis Outline 1 Fatigue theory
- Discussion of fatigue in Al 6061-T6
- Presentation of data sources
- Discussion of effects that modify maximum stress
in fatigue - Discussion of scatter in the maximum stress data
in fatigue - Discussion of multiaxial stress in fatigue
5Analysis Outline 2 Allowable stress
- Determination of allowable stress in fatigue
- Perform a statistical analysis on the MIL-SPEC
data to get confidence curves for a sample set of
fatigue tests. - This yields a starting point for maximum stress
that needs to be corrected for environmental
factors. - The allowable is then compared with the
calculated stress from the FEA results.
6Analysis Outline 3 Calculated Stress
- Description of the finite element model
- FEA results on MH1 and the calculated stresses
- Assumptions
- Thermal analysis
- Magnetic force analysis
- Combined forces transient analysis
- Results for stress ratio R and maximum calculated
stress in horn
7Sources of Fatigue Data for AL 6061-T6 used in
analysis
- MIL-SPEC Handbook 5, Metallic Materials and
Elements for Aerospace Vehicles - ASM Metals Handbook Desk Edition
- ASM Handbook Vol. 19, Fatigue and Fracture
- Aluminum and Aluminum Alloys, pub. by ASM
- Atlas of Fatigue Curves, pub. by ASM
- Fatigue Design of Aluminum Components and
Structures, Sharp, Nordmark and Menzemer
8How well do sources agree?
- For unwelded, smooth specimens, R-1, room
temperature, in air, N5107 - MIL-SPEC smax13 ksi (89.6 MPa)
- Atlas of Fatigue Curves smax17 ksi (117.1 MPa)
- Fatigue Design of Al smax16 ksi (110.2 MPa)
- Metals Handbook (N5108) smax14 ksi (96.5 MPa)
- These numbers represent 50 probability of
failure at 5107 cycles.
9Effects that lower fatigue strength, 1
- Geometry influences fatigue
- Tests are done on smooth specimens and
notched specimens - Smooth specimens have no discontinuities in shape
- Notched specimens have a standard shaped
discontinuity to create a stress riser in the
material - Notches reduce fatigue strength by 1/2
- see graph on next slide
10ASM data showing effect of notches on fatigue
strength
Graph from Atlas of Fatigue Curves
11Effects that lower fatigue strength, 2
- Welding influences fatigue
- Welded and unwelded specimens are tested
- Welding reduces fatigue strength by 1/2
- see graph on next slide
12ASM data showing effect of welding
Graph from Atlas of Fatigue Curves
13Effects that lower fatigue strength, 3
- The stress ratio influences fatigue strength
- Stress Ratio, R, is defined as the ratio of the
minimum to maximum stress. - Tension is positive, compression is negative
- RSmin/Smax varies from -1R1
- R -1 Þ (alternating stress) smax16 ksi
- R 0 Þ (Smin0) smax24 ksi, (1.5X at R-1)
- R .5 Þ smax37 ksi, (2.3X at R-1)
- These values are for N107 cycles, 50 confidence
- Stress ratio is a variable modifier to maximum
stress. Whole stress cycle must be known.
14MIL-SPEC Data Showing Effect of R
This is the page from the MIL-SPEC handbook that
was used for the statistical analysis of the
scatter in fatigue test data. The analytical
model assumes that all test data regardless of R
can be plotted as a straight line on a log-log
plot after all the data points are corrected for
R. The biggest problem with this data
presentation style is that the trend lines
represent 50 confidence at a given life and we
need gt95 confidence of ability to reach 200 x
106 cycles.
15Effects that lower fatigue strength, 4
- Moisture reduces fatigue strength
- For R -1, smooth specimens, ambient
temperature - N108 cycles in river water, smax 6 ksi
- N107 cycles in sea water, smax 6 ksi
- Hard to interpret this data point
- N5107 cycles in air, smax 17 ksi
- See data source on next slide
- Note curve of fatigue crack growth rate in humid
air, second slide
16ASM data on corrosion fatigue strength of many Al
alloys
Graph from Atlas of Fatigue Curves showing that
the corrosion fatigue strength of aluminum alloys
is almost constant across all commercially
available alloys, independent of yield
strength. Data from this graph was used to
determine the moisture correction factor.
17ASM data on effect of moisture on fatigue crack
growth rate
Graph from Atlas of Fatigue Curves This graph
is for a different alloy than we are using, but
the assumption is that moisture probably
increases the fatigue crack growth rate for 6061
also. It was considered prudent to correct the
maximum stress for moisture based on this curve
and the preceding one.
18Discussion of scatter in the maximum stress data
in fatigue
- The MIL-SPEC data is a population of 55 test
specimens that shows the extent of scatter in the
test results. - Trend lines in the original graph indicate 50
chance of part failure at the given stress and
life. - The source gave a method of plotting all the
points on the same curve when corrected for R. - We used statistical analysis to create confidence
curves on this sample set.
19Confidence Curves on Equivalent Stress data plot
This graph plots all of the MIL-SPEC data points
corrected for R by the equation at bottom. The y
axis is number of cycles to failure, the x axis
is equivalent stress in ksi. From this graph we
concluded that the equivalent stress for gt97.5
confidence at 2e8 cycles was 10 ksi.
20Discussion of multiaxial stress in fatigue
- Maximum stress in fatigue is always presented as
result of uniaxial stress tests - Horn stresses are multiaxial.
- We assumed that we could sensibly compare the
uniaxial stress allowable with calculated
multiaxial combined stresses - FEA provided stress intensities and principal
normal stresses that were converted to combined
stress - See next slide for combined stress expression
21Expression for combined stress
- Maximum Distortion Energy Theory provides an
expression for comparing combined principal
normal triaxial stresses to yield stress in
uniaxial tension - We assumed this expression was valid comparing
combined stress with uniaxial fatigue maximum
stress limit - Sallow ³ (S1-S2)2(S2-S3)2(S3-S1)2/2.5
22Allowable Stress Determination 1
- Allowable stress starts as the equivalent stress
for 97.5 confidence that material will not fail
in 2e8 cycles - Seq 10 ksi (68.9 MPa)
- Allowable stress is then corrected by
multiplicative factors, as described in Shigleys
Mechanical Engineering Design - Sallow SeqfRfmoisturefweld
23Calculation of stress ratio correction factor
- First correction is for R,stress ratio
- We determined that the minimum stress was thermal
stress alone after the horn cooled between pulses
just before the next pulse. - Maximum stress happened at time in cycle when
magnetic forces and temperature were peaked
simultaneously - R was calculated by taking the ratio in every
horn element in the FEA of the maximum principal
normal stresses at these two points in time - Results not significantly different for ratios of
combined stress - Smax Seq/(1-R).63 therefore fR 1 /(1-R).63
24Finding the moisture correction factor
- Determining the fatigue strength moisture
correction factor - At R -1, N 108 in river water, smax 6 ksi
- At R -1, N 5108 in air, smax 14 ksi
- 6 ksi/14 ksi .43
- Moisture effect could be .43 smax in air
- We used this number, and assumed that all of the
aluminum was exposed to moisture
25Other Correction Factors
- From data above,
- Welding correction factor, fweld .5
- Welding correction factor only applied to welded
areas - We assumed that there were no notches anywhere.
- This is fair for the inner conductor
- Stresses are so low on the outer conductor that
it doesnt matter - We did not include a size correction to go from
sample size to horn size.
26Description of the finite element model
- We created a 2D axisymmetric model of the horn
and first did a transient thermal analysis - We assumed 3000 W/m2-K convective heat transfer
coefficient all along the inner conductor only - The only heat transfer from the outer conductor
was by conduction to inner - The skin depth of the current was explicitly
modeled (all heat was generated within 1.7mm of
surface of conductors)
27Plot of temperature of smallest radius of inner
conductor vs time
28High Temperature profile in cross-section
The beam axis in the model is a vertical line
(not shown) just to the left of the shape in the
figure
29Conclusions from thermal analysis
- Temperature difference between hot end of pulse
and cool end are not that different. - Heating of the inner conductor elongates it and
pushes end cap along beam axis, putting itself in
compression and the end cap in bending - There are only two areas of the horn that see
significant stress - Middle of the end cap
- Welded region immediately upstream of end cap
30Magnetic Force FEA
- Magnetic forces were modeled in the 2D
axisymmetric model as element pressures using an
analytical expression for the pressure as a
function of radius in the horn. - This model was verified by a 3D 10 sector model
of the horn. - We needed to model the magnetic forces in the 2D
model to be able to combine thermal and magnetic
stress effects.
31Stress intensity caused by high temperature
magnetic force loads on horn end cap
Stress units above are Pascals.
32Conclusions from magnetic thermal analysis
- The magnetic field creates a pressure normal to
the surface the current is flowing through - The magnetic field pressure is non-linear and
maximum at small radii. - Stress ratio in the welded neck is -.16 (low
temperature thermal stress is small compression) - Stress ratio in the end cap varies from -.3 near
beam axis to .5 at middle
33Results of Finite Element Analysis
- The following plot is a graph of the ratio of
calculated principal normal stress to allowable
stress for every element in the horn axisymmetric
model - Stresses have not been combined in this graph
- Values are maximum of S1 and S3 only
- Allowable stress has been derated for moisture
and welding everywhere
34Summary graph for uncombined principal normal
stresses
35Combined Stress Results
- The following graph presents the same results,
but the principal normal stresses have been
combined by the equation shown above - Allowable stress corrected for moisture
everywhere, but welding only where appropriate in
horn - The places where the ratio is gt1 are welded areas
that we have since thickened as a result of this
analysis - Any stress value over 20 of allowable is in the
inner conductor smallest radius tube section
36Summary graph for combined stress data
37Conclusion
- After correcting the thickness of the welded
region upstream of the end cap, the graphs
indicate that the stress level everywhere in the
horn during pulsing is below the maximum set by
the 97.5 confidence level that the material will
not fail in 2e8 cycles.