High Heat Flux Facility GLADIS at IPP Garching
High Heat Flux Facility GLADIS at IPP Garching
High Heat Flux Facility GLADIS at IPP Garching
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<strong>High</strong> <strong>He<strong>at</strong></strong> <strong>Flux</strong> <strong>Facility</strong> <strong>GLADIS</strong> <strong>at</strong> <strong>IPP</strong> <strong>Garching</strong><br />
Outline:<br />
H. Greuner, Ch. Linsmeier, H. Maier<br />
Max-Planck-Institut für Plasmaphysik, Eur<strong>at</strong>om Associ<strong>at</strong>ion, <strong>Garching</strong><br />
1. Introduction & loading conditions in <strong>GLADIS</strong><br />
2. Component oriented investig<strong>at</strong>ions<br />
3. M<strong>at</strong>erial investig<strong>at</strong>ions, surface modific<strong>at</strong>ion of W under H / He beam loading<br />
4. Further facility improvement & summary<br />
Max-Planck-Institut für Plasmaphysik<br />
EURATOM Associ<strong>at</strong>ion<br />
<strong>Facility</strong> designed to evalu<strong>at</strong>e plasma facing components as well as metallic and non-metallic<br />
m<strong>at</strong>erials (W, CFC,…) under fusion relevant he<strong>at</strong> & particle fluxes<br />
<strong>High</strong> he<strong>at</strong> flux test of large actively w<strong>at</strong>er-cooled components as well as small samples<br />
PMI: Investig<strong>at</strong>ion of surface and bulk morphology modific<strong>at</strong>ions of W-PFCs under H/ He loading<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
1
“Where we are”: Experimental activities in the US and Japan<br />
<strong>GLADIS</strong>, high he<strong>at</strong> load & long pulses<br />
600 – 2500 K neutrals<br />
Source: S. Sharaf<strong>at</strong>, UCLA, IAE W‐S<strong>at</strong>ellite ICFRM-14 Sapporo, Sept. 9, 2009<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
2
d<br />
Investig<strong>at</strong>ion of Plasma Facing Components in <strong>GLADIS</strong><br />
<strong>He<strong>at</strong></strong> load resulting from H, He,… particles<br />
plasma facing m<strong>at</strong>erial<br />
externally he<strong>at</strong>ing/ cooling<br />
Lab experiments<br />
Lab experiments,<br />
acceler<strong>at</strong>ors, plasma<br />
devices<br />
m<strong>at</strong>erial, gas<br />
from component<br />
interface<br />
he<strong>at</strong> sink<br />
coolant<br />
actively cooled<br />
T(d) = const.<br />
T(d)<br />
surface<br />
No temper<strong>at</strong>ure gradient<br />
surface<br />
strong temper<strong>at</strong>ure gradient<br />
compressive<br />
tensile<br />
d<br />
compressive<br />
tensile<br />
Surface processes<br />
• depending on T surf (time)<br />
• evapor<strong>at</strong>ion, melting, mixed m<strong>at</strong>erials,<br />
alloys, morphology changes, form<strong>at</strong>ion<br />
of deposited layers, ….<br />
Gas transport into bulk is driven by<br />
• concentr<strong>at</strong>ion gradient<br />
• temper<strong>at</strong>ure gradient<br />
• stress gradient, gas accumul<strong>at</strong>ion in<br />
regions of tensile stress<br />
thermal stress =0<br />
thermal stress<br />
• Component behavior affects the PWI processes and lifetime of component<br />
• Unique investig<strong>at</strong>ions in <strong>GLADIS</strong>, complementary to linear plasma experiments<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
3
1. Introduction <strong>GLADIS</strong> (<strong>Garching</strong> LArge DIvertor Sample test facility)<br />
Neutral beams offer a homogeneous he<strong>at</strong>ing of metallic and non-metallic surfaces (W,<br />
CFC,…) under hydrogen/ helium loading conditions.<br />
• 2010: start of oper<strong>at</strong>ion of 2nd beam line, completely independent oper<strong>at</strong>ion<br />
Free superposition of the two beams possible!<br />
Unique capability for oper<strong>at</strong>ion with H, He or mixed H/He neutral beams and thermal loads<br />
• Power 2 x 1 MW ion source, H 2<br />
• U ex 15 – 55 KV<br />
• <strong>He<strong>at</strong></strong> flux 3 - 45 MW/m²<br />
• Loaded area 300 cm²<br />
• Pulse length 1 ms - 45 s<br />
• Cycle r<strong>at</strong>e 80 - 100 /h<br />
• Target dim. up to 2 m<br />
using vacuum lock)<br />
• Target cooling: (currently)<br />
(0.6 m<br />
„high purity w<strong>at</strong>er“ fulfils ITER requirements<br />
flow r<strong>at</strong>e: ≤ 8.5 l/s (T‘=20 °C)<br />
1 MW ion<br />
sources<br />
~ 3700<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
4<br />
1800<br />
target plane
Physical parameters and loading conditions<br />
<strong>He<strong>at</strong></strong> flux distribution <strong>at</strong> target position<br />
(examples)<br />
corresponding H/ He particle flux:<br />
<strong>He<strong>at</strong></strong> load H: φ Η , [m -2 s -1 ] He: φ He , [m -2 s -1 ]<br />
2 MW/m² 0.7 · 10 21 0.75 · 10 21<br />
10 MW/m² 2.5 · 10 21 2 · 10 21<br />
Calcul<strong>at</strong>ed penetr<strong>at</strong>ion depth of particles<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
5
Current programme: Main achievements of component tests<br />
W7-X: highly loaded divertor pl<strong>at</strong>es: (production ongoing)<br />
• 15 m² target area, 900 actively cooled CuCrZr<br />
elements,CFC NB31 covered, Σ 18,000 CFC tiles<br />
60 prototypes tested, focused on reliability of CFC/Cu<br />
interlayer, finally 99.4% of tested tiles w/o defects<br />
• up to 10,000 cycles 10 MW/m², 10 s<br />
• screening 32 MW/m², 30 s, and CHF tests 31 MW/m²<br />
JET ILW: W Co<strong>at</strong>ings on CFC (fibre-reinforced carbon)<br />
• R&D and quality assurance for 50 m² inner wall<br />
• Evalu<strong>at</strong>ion tests mainly performed in <strong>GLADIS</strong><br />
– Upscaling of VPS process to real size failed<br />
– PVD W/Re multilayer caused problems<br />
beam dump<br />
target length 600 mm<br />
W7-X Manufactured target test by (view PLANSEE from the (Austria) ion source)<br />
10 µm thin W magnetron sputter co<strong>at</strong>ing on Mo interlayer,<br />
150 mm<br />
was finally selected<br />
W-PVD co<strong>at</strong>ing on CFC during he<strong>at</strong> loading<br />
• further physical investig<strong>at</strong>ion, carbide form<strong>at</strong>ion & brittleness, life-time…<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
6
Investig<strong>at</strong>ion of W Plasma Facing Components for DEMO<br />
Physics topics:<br />
• Investig<strong>at</strong>ion of surface and bulk morphology modific<strong>at</strong>ions of W PFCs which have both,<br />
high he<strong>at</strong> and simultaneous high particle loading similar to the expected ITER /DEMO<br />
loading conditions primary H, He (5 – 100%), impurities N, Ar,..<br />
Collabor<strong>at</strong>ions:<br />
• EFDA topical group m<strong>at</strong>erials: investig<strong>at</strong>ion of W and W alloys<br />
• KIT - He cooled W divertor: investig<strong>at</strong>ion of erosion, micro-cracks<br />
Example of performed investig<strong>at</strong>ions in 2010:<br />
focussed on He loading under divertor conditions<br />
test of different manufactured W m<strong>at</strong>erials provided by <strong>IPP</strong> & FZJ<br />
study of temper<strong>at</strong>ure and fluence dependence<br />
Loading conditions: Φ= 1·10 24 – 3·10 25 He/m²<br />
he<strong>at</strong> flux: 10 - 15 MW/m²<br />
T surf = 600 - 1550°C (depending on height of sample)<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
7
He beam loading of actively cooled component<br />
<strong>He<strong>at</strong></strong> load distribution and resulting surface temper<strong>at</strong>ures<br />
Rolled pl<strong>at</strong>e<br />
Rod Ø12 mm<br />
Forged pl<strong>at</strong>e Rod Ø30 mm<br />
Rod Ø80 1 2 3 mm 4 Rod Ø30 mm (POLEMA)<br />
Rod Ø60 mm<br />
cooling w<strong>at</strong>er<br />
15 mm: 1550 °C<br />
10 Height: mm: 1000 5 -15 °C mm<br />
Temper<strong>at</strong>ure distribution:<br />
15 mm W tile with 10 MW/m²,<br />
12 m/s cooling w<strong>at</strong>er, 20°C,16bar<br />
applied particle fluences:<br />
tile 1, 4: loaded with 1· 10 24 He/m²<br />
tile 2,3: loaded with 1· 10 25 He/m²<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
8
Tsurf=200°C<br />
Results: influence of surface temper<strong>at</strong>ure on erosion (1)<br />
high fluence 1·10 25 He/m²<br />
1 µm<br />
note: 70 nm penetr<strong>at</strong>ion depth<br />
Tsurf=1000°C<br />
calcul<strong>at</strong>ed erosion: 5 µm<br />
Low temper<strong>at</strong>ure: no bubble form<strong>at</strong>ion was observed<br />
Tsurf ≥ 1000°C: strong bubble form<strong>at</strong>ion domin<strong>at</strong>es erosion p<strong>at</strong>tern<br />
Tsurf=1450°C<br />
Further investig<strong>at</strong>ion: confirm<strong>at</strong>ion of results, determin<strong>at</strong>ion of “bubble start temper<strong>at</strong>ure”<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
9<br />
1 µm<br />
1 µm<br />
FIB cross-sections M.Balden
Results: influence of particle fluence on erosion (2)<br />
constant surface temper<strong>at</strong>ure 1000°C<br />
1·10 24 He/m²<br />
calcul<strong>at</strong>ed erosion: 0.5 µm<br />
1 µm<br />
No pronounced dependence on fluence<br />
Surface degrad<strong>at</strong>ion occurred after very low fluence<br />
Balance between bubble form<strong>at</strong>ion and erosion r<strong>at</strong>e<br />
1·10 25 He/m²<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
10<br />
1 µm<br />
calcul<strong>at</strong>ed erosion: 5 µm<br />
FIB cross-sections M.Balden
Summary He loading<br />
Helium loading:<br />
Morphology domin<strong>at</strong>ed by physical sputtering due to He.<br />
For lower temper<strong>at</strong>ures the erosion p<strong>at</strong>terns depend on the local orient<strong>at</strong>ion of each individual grain.<br />
T surf < 850°C Cone and wave structures for long pulses and high fluence, loss of micro particles<br />
T surf 1000 – 1500°C Form<strong>at</strong>ion of sharp cone like structures; nano-sized bubbles inside cones<br />
no pronounced dependence on fluence or surface temper<strong>at</strong>ure<br />
T surf > 2000°C Form<strong>at</strong>ion of coral-like structures with depth of several µm<br />
Conclusions:<br />
• He bombardment modifies the surface stronger as expected<br />
• results in higher erosion r<strong>at</strong>e and possible dust production<br />
• but: no c<strong>at</strong>astrophic effects expected concerning lifetime of plasma facing m<strong>at</strong>erial<br />
• <strong>at</strong> present no consistent explan<strong>at</strong>ion of form<strong>at</strong>ion mechanism of all observed structures available.<br />
Further investig<strong>at</strong>ions are necessary, especially effects of mixed H/He loading (in progress)<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
11
Future technical capabilities<br />
KIT: strong interest in cooper<strong>at</strong>ion for PF m<strong>at</strong>erial investig<strong>at</strong>ions in the frame of<br />
DEMO divertor development<br />
• Advanced W based alloys developed by KIT,<br />
• Armour m<strong>at</strong>erial optimiz<strong>at</strong>ion of divertor modules<br />
Proposed Upgrade to meet DEMO cooling conditions:<br />
• Under discussion ~2011-2013<br />
Hot He coolant loop:<br />
• He loop: 130 g/s He flow, p=80 bar, 400-430°C<br />
• vessel modific<strong>at</strong>ions, auxiliary equipment<br />
He-cooled modular divertor<br />
P.Norajitra, ICFRM 14<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
12
Summary<br />
• <strong>GLADIS</strong> is a well-characterized and reliable NB facility<br />
• Sensitive diagnostics for both beams and samples during loading<br />
• Oper<strong>at</strong>ion with 2 independent beams allows superposition of various he<strong>at</strong> and<br />
particle loading<br />
• Investig<strong>at</strong>ion of small m<strong>at</strong>erial samples as well as full-scale w<strong>at</strong>er-cooled<br />
components complementary to linear plasma devices<br />
• <strong>GLADIS</strong> embedded in <strong>IPP</strong> M<strong>at</strong>erials Research division<br />
• Additional m<strong>at</strong>erial characteriz<strong>at</strong>ion expertise and equipment available<br />
H. Greuner, <strong>IPP</strong> <strong>Garching</strong> PMTS Workshop, Aug.31 –Sep.2 2010<br />
Oak Ridge, TN, USA<br />
13