Abstract:Heat loads of 10MW m-2 are expected for steady state operation at ITER and up to 20MW m-2 in slow transient situations. Plasma linear devices like Magnum-PSI can recreate situations close as those expected to be achieved at ITER divertor, providing easier access for diagnostics than in a tokamak. Numerical models are still necessary to complement experiments and to extrapolate relevant information to fusion devices, as the relevant Atomic and Molecular (A\&M) processes. SOLPS-ITER (formerly known as B2.5-E… Show more
“…Once all of this is taken into account, the solid TZM case is produced as shown in figure 8. A good agreement between the simulation with SOLPS-ITER, which uses D as the main species, and the hydrogen calibration experimental shot is found, although electron density is slightly lower than in experiments, but still in an acceptable margin as in previous cases [40]. Additionally, this result is in good agreement with the experimental 200 • C solid TZM case, meaning that the use of a hydrogen shot in similar conditions to obtain upstream boundary conditions is a valid method if no source TS measurements…”
Section: Numerical Setupsupporting
confidence: 62%
“…The target is assumed to have a 100% recycling of deuterium and lithium ions. During the solid target simulations, this assumption has been used in the past [39,40], while for the porous target it is assumed that the temperature is too high for the Li to retain D. The plasma flux reaching the edge of the beam is automatically recombined and acts as a source of neutral particles in Eirene, i.e. there are no ions outside the plasma beam.…”
The vapor-box is a liquid metal based design to cope with the demanding conditions of the divertor. This design relies on the recirculation of lithium by evaporation and condensation. An issue to this approach is the safety risks of Li-D/T formation and co-deposition on both the vapor-box walls - leading to possible recirculation impedance- and on the first wall leading to unacceptable tritium retention. Additively manufactured tungsten Capillary Porous Structure (CPS) samples filled with Li were exposed to high heat flux D plasmas in the linear plasma device Magnum-PSI and Li-D co-deposition was measured as a function of substrate temperature, estimated to be in the range 200-428 ${^\circ}$C and distance between 25-85 mm to the plasma beam center. The D:Li ratio was determined via in-situ ion beam diagnostics (NRA and EBS) and the spectra analyzed simultaneously to maximise the precision of the measurement. The experimental results approach close to the theoretical maximum at 40:60 D:Li ratio and the thickness of the deposited films was 0.02 - 3.2 $\mu$m. For witness plate temperatures above 400 ${^\circ}$C Li films under 150 nm in thickness were deposited and show lower D:Li ratios, as low as 5:95 D:Li ratio. At these temperatures the evaporation rate from the WPs is close to the deposition rate, and the decomposition pressure for LiD becomes comparable to the operational pressure in the vessel during the discharge. SOLPS-ITER simulations were also conducted to complement the experimental data. The results were used to narrow the range of CPS surface temperature to between $650-700$^{\circ}$C and determined that the D$^{+}$ plasma is largely replaced by Li$^{+}$ plasma close to the target surface. Further, the redeposition ratio of the lithium on the CPS surface is determined to be around 80$\%$, which matches well with the value determined from a quartz crystal microbalance. Due to limitations in the modeling of neutral interactions with Li coated surfaces, the SOLPS-ITER modeling does not well recreate the observed Li and D deposition layers on the WPs, indicating that this aspect of the modeling in Eirene needs improvement to accurately model plasmas containing significant quantities of Li. However, SOLPS-ITER simulations should be extended to include LiD molecules and improve the accuracy of heat flux towards the target to improve the comparison with experimental data.
“…Once all of this is taken into account, the solid TZM case is produced as shown in figure 8. A good agreement between the simulation with SOLPS-ITER, which uses D as the main species, and the hydrogen calibration experimental shot is found, although electron density is slightly lower than in experiments, but still in an acceptable margin as in previous cases [40]. Additionally, this result is in good agreement with the experimental 200 • C solid TZM case, meaning that the use of a hydrogen shot in similar conditions to obtain upstream boundary conditions is a valid method if no source TS measurements…”
Section: Numerical Setupsupporting
confidence: 62%
“…The target is assumed to have a 100% recycling of deuterium and lithium ions. During the solid target simulations, this assumption has been used in the past [39,40], while for the porous target it is assumed that the temperature is too high for the Li to retain D. The plasma flux reaching the edge of the beam is automatically recombined and acts as a source of neutral particles in Eirene, i.e. there are no ions outside the plasma beam.…”
The vapor-box is a liquid metal based design to cope with the demanding conditions of the divertor. This design relies on the recirculation of lithium by evaporation and condensation. An issue to this approach is the safety risks of Li-D/T formation and co-deposition on both the vapor-box walls - leading to possible recirculation impedance- and on the first wall leading to unacceptable tritium retention. Additively manufactured tungsten Capillary Porous Structure (CPS) samples filled with Li were exposed to high heat flux D plasmas in the linear plasma device Magnum-PSI and Li-D co-deposition was measured as a function of substrate temperature, estimated to be in the range 200-428 ${^\circ}$C and distance between 25-85 mm to the plasma beam center. The D:Li ratio was determined via in-situ ion beam diagnostics (NRA and EBS) and the spectra analyzed simultaneously to maximise the precision of the measurement. The experimental results approach close to the theoretical maximum at 40:60 D:Li ratio and the thickness of the deposited films was 0.02 - 3.2 $\mu$m. For witness plate temperatures above 400 ${^\circ}$C Li films under 150 nm in thickness were deposited and show lower D:Li ratios, as low as 5:95 D:Li ratio. At these temperatures the evaporation rate from the WPs is close to the deposition rate, and the decomposition pressure for LiD becomes comparable to the operational pressure in the vessel during the discharge. SOLPS-ITER simulations were also conducted to complement the experimental data. The results were used to narrow the range of CPS surface temperature to between $650-700$^{\circ}$C and determined that the D$^{+}$ plasma is largely replaced by Li$^{+}$ plasma close to the target surface. Further, the redeposition ratio of the lithium on the CPS surface is determined to be around 80$\%$, which matches well with the value determined from a quartz crystal microbalance. Due to limitations in the modeling of neutral interactions with Li coated surfaces, the SOLPS-ITER modeling does not well recreate the observed Li and D deposition layers on the WPs, indicating that this aspect of the modeling in Eirene needs improvement to accurately model plasmas containing significant quantities of Li. However, SOLPS-ITER simulations should be extended to include LiD molecules and improve the accuracy of heat flux towards the target to improve the comparison with experimental data.
Self-healing liquid metal divertors (LMDs) based on the Capillary Porous Structure (CPS) concept are currently being considered among the possible solutions to the power exhaust problem in future fusion reactors. Indeed, the passive replenishment of the plasma-facing surface by capillary forces and the self-shielding of the target via vapor emission can potentially improve the divertor lifetime and its resilience to transient loads. On the other hand, the LMD target erosion can be significant due to evaporation and thermal sputtering, on top of physical sputtering, possibly leading to unacceptable core plasma dilution/power losses (for a low-Z/high-Z metal such as Li and Sn, respectively). For this reason, it is necessary to assess whether an LMD is compatible with an European DEMO (EU-DEMO) plasma scenario. This requires a self-consistent model of the impurity emission from the target, the plasma in both the scrape-off layer (SOL) and the core regions and the transport of impurities therein. In this paper, an an integrated modelling approach is proposed, which is based on SOLPS-ITER and includes its coupling with a target erosion model written in FreeFem++ and a core plasma model (ASTRA/STRAHL). An application of the coupled SOL-target model to simulate experiments performed in the Magnum-PSI linear plasma device with a CPS target filled with Li is also included to provide a first demonstration of the capabilities of the approach. Results are promising, being in good agreement (within a few degrees) with the measured target temperature distribution. In perspective, the modelling framework presented here will be applied to the EU-DEMO with an Sn divertor.
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