May 28-29, 2008/ARR 1 Thermal Effect of Off-Normal Energy Deposition on Bare Ferritic Steel First Wall A. René Raffray University of California, San Diego.

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Presentation transcript:

May 28-29, 2008/ARR 1 Thermal Effect of Off-Normal Energy Deposition on Bare Ferritic Steel First Wall A. René Raffray University of California, San Diego ARIES Meeting UW, Madison, WI May 28-29, 2008

May 28-29, 2008/ARR 2 Power Plant FW Under Energy Deposition from Off- Normal Conditions Thermal impact of off-normal events on power plant FW presented before for SiC and W Questions arise as to the possibility of utilizing a bare FS FW in a power plant ARIES has considered the bare wall possibility in previous design studies but not clear whether the plasma interaction and possible contamination issue would be acceptable Thermal effect on FS FW investigated

May 28-29, 2008/ARR 3 Off-Normal Thermal Loads for Analysis with RACLETTE Code From ITER (from PID and C. Lowry’s presentation at 2007 ITER WG8 Design review Meeting) Disruptions: –Parallel energy density for thermal quench = MJ/m 2 near X-point –Deposition time ~ 1-3 ms –Perpendicular energy deposition will be lower, depending on incidence angle (at least 1 order of magnitude lower) –Parallel energy deposition for current quench = 2.5 MJ/m 2 -For power plant, fusion energy is ~ 4x higher than ITER and the energy deposition will also be higher -Parametric analysis over 1-10 MJ/m 2 and 1-3 ms VDE’s: –Energy deposition = 60 MJ/m 2 –Deposition time ~ 0.2 s ELMS: –Parallel energy density for thermal quench (controlled/uncontrolled) ~ 0.77/3.8 MJ/m 2 –Deposition time ~ 0.4 ms –Frequency (controlled/uncontrolled) = 4/1 Hz -Assumed power plant case ~0.3/1.5 MJ/m 2 incident energy deposition over 0.4 ms

May 28-29, 2008/ARR 4 Vapor Pressure and Thermal Properties of FS MANET properties assumed for ferritic steel (from Panayiotis J. Karditsas and Marc-Jean Baptiste) Heat of evaporation = kJ/kg Heat of fusion = kJ/kg Melting point = °C k = W/m-K P vap (Pa) = 10 ( /T(K))

May 28-29, 2008/ARR 5 Example Disruption Case for Power Plant with Bare FS FW Disruption simulation: q''=1.667 x 10 9 W/m 2 over 3 ms (~5 MJ/m 2 )4+1 mm FS FW Cooled by He at 483°C with h = 5.2 kW/m 2 -K 5-mm FS He h = 5.2 kW/m 2 -K T = 483°C Energy Deposition

May 28-29, 2008/ARR 6 Parametric Study of Maximum Phase Change Thickness of a FS FW Temperature for Different Disruption Scenarios (DCLL Case) 4+1 mm FS FW cooled by He at 483°C with h = 5.2 kW/m 2 -KUp to ~0.1 mm melt layer and ~0.1 mm evaporation loss per event Only a few events allowable based on erosion lifetime depending on energy density 5-mm FS He h = 5.2 kW/m 2 -K T = 483°C Energy Deposition

May 28-29, 2008/ARR 7 Parametric Study of Maximum Temperature of FS FW for Different Disruption Scenarios (DCLL Case) 4+1 mm FS FW cooled by He at 483°C with h = 5.2 kW/m 2 -K 5-mm FS He h = 5.2 kW/m 2 -K T = 483°C Energy Deposition

May 28-29, 2008/ARR 8 Example VDE Case for Power Plant with FS FW VDE simulation: q''= 3 x 10 8 W/m 2 over 0.2 s (60 MJ/m 2 )4+1 mm FS FW cooled by He at 483°C with h = 5.2 kW/m 2 -KEven 1 event is not acceptable (complete loss of armor)Same conclusions previously for W and SiC armor

May 28-29, 2008/ARR 9 Example Uncontrolled ELM Case for Power Plant with FS FW ELM simulation: q''= 3.75 x 10 9 W/m 2 over 0.4 ms (1.5 MJ/m 2 )4+1 mm FS FW cooled by He at 483°C with h = 5.2 kW/m 2 -K~0.1 melt layer and ~0.01 mm evaporation loss per event (1 Hz frequency) Not acceptable (complete loss of armor after such events)From previous study, also not acceptable for SiC (~0.02 mm armor loss per event) and W armor (5x10 -5 melt layer and 3x10 -7 evaporation loss per event)

May 28-29, 2008/ARR 10 Example Controlled ELM Case for Power Plant with SiC FW ELM simulation: q''= 7.5 x 10 8 W/m 2 over 0.4 ms (0.3 MJ/m 2 )4+1 mm FS FW cooled by He at 483°C with h = 5.2 kW/m 2 -K~10 -5 m melt layer and and <10 -9 m evaporated thickness per event (5 Hz frequency) Complete loss of 1-mm FS armor after such events, depending on stability of melt layer (at best ~55 hours if occurring at same location) - Not acceptableFrom previous study, also not acceptable for SiC (~0.08  m of armor loss per event or ~ 1 month of operation ) but probably ok for W armor (T max =1872°C; no melt; m evaporation loss per event)

May 28-29, 2008/ARR 11 Summary of Assessment of Off-Normal Energy Deposition on FS FW (DCLL like) (based on assumed scenarios) Focus on thermal effects EM effects will also be important for DCLL FS FW Only a few disruptions can be accommodated (depending on the energy density) VDE cannot be accommodated Only limited number of uncontrolled ELM cases can be accommodated Controlled ELM’s would drastically limit the lifetime of FS armor (a few days) but might be acceptable for W armor based on previous study Avoidance or mitigations of disruptions (and off-normal events) is a key requirement for power plant applications