Fatigue Lifetime Measurements on Tungsten Wires Subject to Repeated Thermal Stress J. R. J. Bennett 1 , J. Back 2 , S. Brooks 1 , R. Brownsword 1 , A. Crossley 3 , C. J. Densham 1 , R. Edgecock 1 , S. Gray 1 , A. J. McFarland 1 , C. Salter 3 and G. Skoro 4 1 Rutherford Appleton Laboratory, Harwell Science and Innovation Campus, Didcot, Oxon. OX11 0QX, UK 2 Department of Physics, University of Warwick, Coventry. CV4 7AL, UK 3 BegbrokeNano, Oxford Materials Characterisation Services, Oxford University Begbroke Science Park, Sandy Lane, Yarnton. Oxon. OX5 1PF, UK 4 Department of Physics and Astronomy, University of Sheffield, Sheffield. S3 7RH, UK [email protected]3rd High-Power Targetry Workshop 10-14 September 2007 Bad Zurzach Switzerland
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Fatigue Lifetime Measurements on Tungsten Wires Subject to Repeated Thermal Stress
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Fatigue Lifetime Measurements on Tungsten Wires Subject to Repeated Thermal StressJ. R. J. Bennett1, J. Back2, S. Brooks1, R. Brownsword1, A. Crossley3, C. J.
Densham1, R. Edgecock1, S. Gray1, A. J. McFarland1, C. Salter3 and G. Skoro4
1Rutherford Appleton Laboratory, Harwell Science and Innovation Campus, Didcot, Oxon. OX11 0QX, UK2Department of Physics, University of Warwick, Coventry. CV4 7AL, UK
3BegbrokeNano, Oxford Materials Characterisation Services, Oxford University Begbroke Science Park, Sandy Lane, Yarnton. Oxon. OX5 1PF, UK
4Department of Physics and Astronomy, University of Sheffield, Sheffield. S3 7RH, UK
Schematic circuit diagram of the wire test equipment
turbopump
Penning gauge
window
window
test wire
ISO 63 teebulkhead high voltage
feed-throughs
ct
Schematic section of the wire test assembly
8 Co-axial cables
Top plate
ISO 63 cross
4 support rods
Electrical return copper strip
Vertical Section through the Wire Test Apparatus
Current
Inner conductor of co-axial insulator feed-through.
Stainless steel split sphere
Copper “nut”
Current
Two graphite (copper) wedges
Tungsten wire
Spring clips
Fixed connection
Sliding connection
W26
Tungsten Wire
Assembly
Picture of the pulse current, 200 ns/division
Picture of the pulse current, 1 μs/division
Picture of the wire test equipment
Measurement of the Pulse Temperature1 kHz measurement rate
Tests on Tantalum WireThe wire lasted for a few hundred thousand pulses before breaking or bending.
Tantalum is not a suitable material since it too weak at high temperatures (1600-2000 K).
Photograph of the tantalum wire showing characteristic wiggles before failure.
Yield and Ultimate Strength of Tantalum and alloys versus Temperature.
Yield
Ultimate
Yield Yield
Ultimate
Ultimate
Yield Strength of Tungsten and some Alloys versus Temperature
Ulti
mat
e Te
nsile
Stre
ngth
, MP
a
Ultimate Tensile Strength of Tungsten and some Alloys versus Temperature
Tests on Tungsten WireTungsten is much stronger than Tantalum particularly at high temperatures.
So - try Tungsten
Equivalent Power, MW, in Target
Diameter
Target Number
Pulse Current
A
Temp Jump
K
Peak Temp
K
Number of Pulses to Failure
Comments
2 cm 3 cmW03 4900
720090
20020002200
>3.4x106
16,500 BrokeBroke2.35
4.810
W08 6400 150 1900 >1.6x106 Wire stuck to top connection
(cu blocks)
3.9 8.4
W09 55605840
120130
19002050
4.2x106
9x106Top connector
failed3
3.36.47.0
W15 6400 180 1950 1.3x106 Wire stuck to top connection
(cu blocks)
3.9 8.4
W26 62007520-8000
140~230
2000~1800
10x106
3x106 BrokeBroke3.6~6
7.8~12
W28
W30
6560
4720
180
93
1900
1870
26.4x106
>54.5x106
Crack appearedCrack appeared
Not brokenNot broken
4.1
2.2
8.8
4.5
Some Results: 0.5 mm diameter Tungsten Wires
“Equivalent Target”: This shows the equivalent beam power (MW) and target radius (cm) in a real target for the same stress in the test wire. Assumes a parabolic beam distribution and 3 micro-pulses per macro-pulse of 20 micro-s.
Radiation Damage1. Experience on the ISIS targets show that
there is no serious problem up to ~12 dpa.
2. Tungsten pellets irradiated (~15-20 dpa) at PSI will be examined when cool enough.
3. Tests at BNL, (Nick Simos).
SEM ANALYSIS OF 4 SAMPLES OF TUNGSTEN WIRE.
Chris SalterWith the aim to observe any surface or internal damage which might indicate the presence of thermal fatigue. Micro-cracks can indicate fatigue.
Samples. 4 wires were supplied, W31 to W34.
The following techniques were used to characterise the samples:• SEM imaging of the wires as delivered using both the secondary electron and the back-scattered electron signal.• Some energy dispersive analysis to determine the nature of some of the features observed.• The same samples were mounted in cold setting resin and polished, again observed using the SEM.
Results and Discussion
Wire W31; Unbroken wireAn extensive search found no surface signs of any fatigue cracks. However, the surface of the tungsten wire had been thermally etched in the central region, with extensive removal of material from the grain boundary regions.Also, No signs of cracks in the sections.
Wire W32 and 33; Broken.No signs of fatigue micro-cracks. But wire severely melted at brake.
Wire W34; Crack just appeared in thermal test, Broke on cooling.
Massive cracking near the brake in the wire. Is this a sign of fatigue stress?
W34
W34. Showing cracking at surface behind the main fracture surface, still in necking zone.
W 34. Section
W34. Section
W34. Section
ConclusionsI believe that the viability of solid tungsten targets at high-temperature for a long life (~10 years) has been demonstrated with respect to thermal shock and fatigue and will not suffer undue radiation damage.
Future Programme1. Continue wire tests with Tungsten and Graphite.2. Continue modelling computations.3. Continue SEM measurements.4. VISAR measurements to asses the properties of tungsten,
and any changes, during the wire tests. (Effect of thermal shock.)
5. Tests with a proton beam to confirm wire tests and VISAR measurements – but limited number of pulses.
6. Radiation damage studies.7. Test alloys of tungsten.8. Design & build a model of the target bar system.9. Design the solenoid.10.Design and cost the complete target station including the