1 / 16

The new ITER-like Wall in-vessel components

The new ITER-like Wall in-vessel components. What are the constraints?. W-coated CFC: Risk factor: carbidisation… interlayer embrittlement… failure Limit steady state to 1200 o C initially Limit transients to 330 kJ/m 2 to be confirmed Be: Risk factor: melting ~1240 o C

radha
Download Presentation

The new ITER-like Wall in-vessel components

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. The new ITER-like Wall in-vessel components

  2. What are the constraints? W-coated CFC: Risk factor: carbidisation… interlayer embrittlement… failure Limit steady state to 1200o C initially Limit transients to 330 kJ/m2 to be confirmed Be: Risk factor: melting ~1240oC Limit steady state to 950oC Limit transients to 20 MJ/m2/s1/2 from literature Bulk W: Risk factor: crystallization Limit steady state surface to 1200oC initially, 2200oC later on possibly (this takes stressed region to 1200oC) Risk factor: macro deformation, UFO… Limit springs to 350oC or 60 MJ/m2 (with TWF=1) Limit transients to 20 (MJ/m2)/s1/2 from literature Min density for NBI Compatible with ohmic limiter phase Generous GAPS initially Caution with RF/LH localised load Max ELM size

  3. Bulk W LBSRP • Surface temperature limit: initially 1200oC (avoid recrystallisation), later 2200oC • Wedge temperature (600oC, or 72 MJ/m2) • Springs (under investigation, probably 350oC, or <60 MJ/m2)… sweeping might be necessary • ELMs (literature) 20 MJ/m2/s1/2

  4. Bulk W LBSRP P Lomas + S Jachmich Toroidal wetted area affected by: gaps between stacks and their shadowing, gaps between lamella and their shadowing. Toroidal conductivity within stack very small: heat goes straight down to springs.

  5. Bulk W LBSRP MARION tests at >58 MJ/m2 with thermal barrier above spring (stack 1-2-3) confirm this is sufficient to stay <330oC, stack 4 to be investigated. P Mertens et al

  6. W-coated divertor tiles • Surface temperature limit: initially 1200oC • Energy limit ~unchanged (minor effect on inter-pulse cooling, low e) • ELMs (under investigation)

  7. W-coated divertor tiles - ELMs 100x, 1 ms long, JUDITH shots C Thomser et al

  8. W-coated divertor tiles - ELMs 100x, 1 ms long, JUDITH shots C Thomser et al

  9. Be inner top: Melting: MIGHT be limiting with high triangualrity, high proximity of second X-point, high flux expansion… Be inner and outer limiter: Melting: OK with ohmic ramp-up and ramp-down OK with sufficiently large gaps Incompatible with plasma contact during heating phase MIGHT suffer with localised RF loads Beryllium main chamber Limiter – bidirectional / Divertor - unidirectional

  10. Beryllium operational limits Max input power has been estimated for 5 DESIGN LIMITER configurations and 3 X-point configurations to stay within Be melting limits CEA under TA Constant: 6 MW/m2 x 10 s OR 8.4 MW/m2 x 5 s Ramp (to/from): 10 MW/m2 x 10 s OR 14 MW/m2 x 5 s

  11. Be: ohmic ramp up+down always OK Assuming power always peaks on the same tile, which will not be the case. Power density can be translated in surface temperature for “any” loss power (t):

  12. … a generic problem of high triangularity scenarios Be: high-d X-point might overload SC V_4M5_LT: OK everywhere 3MA5_HT3: high loads on SC(UI) and DP – not cured analytically so far 3MA5_ITER: high loads on SC(UI) – not cured analytically so far 3MA5_ITER: high loads outer wall – OK if ROG increased by 1 cm

  13. Beryllium transient limits Be melt threshold ~20 MJ/m2/s1/2 Unlikely to have ELMs with such a severity in the main chamber Disruptions of sufficient severity are possible V Riccardo and A Loarte, NF 45, p.1427-1438 C1-C19 Residual fraction only for PTN energy >1 MJ Fast ITB collapses now rare, but not completely vanished (4 in 2009)

  14. Neutral beams • Normal bank (IWGL+IWC): • Surface temperature limit on W-coated CFC tiles • Bulk temperature limit on fixings and W-coating at cork (60 MJ/m2) • Tangential bank (various inner and outer wall locations): • Be melting (IWGL apex + WPL) • Surface temperature limit on W-coated CFC tiles (IWGL wing + SC trays +… ) • pre-existing weak points (knuckles, bolts… ) same or improved limits Where are the ILW constraints?

  15. Inner wall NBI footprints Outer wall NBI footprints Colour code (typical): W-coated CFC and berylliumPower density on footprint edge: 0.5 and 1.0 MW/m2 NBI revised operational limits

  16. What are the constraints? W-coated CFC: Risk factor: carbidisation… interlayer embrittlement… failure Limit steady state to 1200o C initially Limit transients to 330 kJ/m2 to be confirmed Be: Risk factor: melting ~1240oC Limit steady state to 950oC Limit transients to 20 MJ/m2/s1/2 from literature Bulk W: Risk factor: crystallization Limit steady state surface to 1200oC initially, 2200oC later on possibly (this takes stressed region to 1200oC) Risk factor: macro deformation, UFO… Limit springs to 350oC or 60 MJ/m2 (with TWF=1) Limit transients to 20 (MJ/m2)/s1/2 from literature Min density for NBI Compatible with ohmic limiter phase Generous GAPS initially Caution with RF/LH localised load Max ELM size

More Related