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Managing Tritium Inventory and Permeation in In-Vessel Systems

This article discusses the challenges of managing tritium inventory and permeation in in-vessel systems for ITER and DEMO. It covers factors that affect fuel retention, tritium diffusion, and radiation-specific effects. Laboratory experiments and recent research findings are explored to provide insights into tritium trapping, retention, and permeation in different materials. The article also proposes potential research directions for further investigation.

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Managing Tritium Inventory and Permeation in In-Vessel Systems

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  1. Managing in-vessel tritium inventory and permeation presents a significant technical challenge for both ITER and DEMO • Scope: • Each 400 s ITER pulse uses 120 g of T2 (1.2×106 Ci) • Release limit: 1 Ci/day; Release fraction <10-6 for one shot • Limited Experience: 99 g processed during TFTR D-T campaign • Self-fuel sufficiency requires retention < 0.01% [Tanabe, J. Nucl. Mater. (2013)] • Fuel retention closely coupled with several other factors: • Plasma conditions (flux, fluence, surf. temp., etc.) • Material microstructure • Concentration and type of intrinsic defects within material • Plasma-induced damage (H and He precipitates) • Defects introduced through neutron bombardment • Tritium/Radiation-specific effects: • Enhancement of T diffusion in a radiation environment. • Atomic T can circumvent permeation barriers that block T2 dissociation / chemisorption • 3He accumulation in material / 3He(n,H)Trecoils with E = 100’s keV • Different trap energies, diffusion constants, etc. Tritium inventory in ITER for various PFC options [J. Roth et al., Plasma Phys. Control. Fusion (2008).]

  2. Laboratory experiments have provided insight into physics governing hydrogen trapping in un-damaged W • Fluence and temperature dependence extensively explored since the 1990’s. • Absolute values vary considerably between laboratories, but several clear trends can be discerned. Fluence Dependence*: PISCES-B exposures confirm t1/2 scaling, but no saturation* • Temperature Dependence*: • (a) Low D retention at T < 200 °C • Slow kinetics, i.e. permeation. • (b) Max. D retention at 300 - 400 °C • Traps fill and diffusion is fast enough to extend to greater depths. • (c) Low D retention at T > 400 °C • Weak binding of D to traps. a b c T=640 K *W. R. Wampler, Int. H Workshop (2010.) Summary of retention data (temperature dependence) • H plasma flux and ion energy: • Affect near-surface concentration at the end of range • Have a less pronounced effect on hydrogen diffusion and retention *R. Doerner et al, Nucl. Mater. Energy (2016)

  3. Retention will be strongly influenced by evolving material microstructure • Effect of specimen microstructure: • Different intrinsic defects for trapping • Strongly coupled to blister and bubble nucleation and growth (trap H2 gas, reduce H permeation into the bulk) • Diffusion enhancement and trapping along grain boundaries • Modification by low energy H plasma: precipitate growth suppressed blistering loop punching blistering Retention in different tungsten grades varies ~ 20x M. Balden, et al J. Nucl. Mater. 2014 rolled W ultra-fine grained W R. Kolasinski, et al Int. J. Ref. Met. & Hard Mater. (2016) recrystallized W ITER-grade W S. Lindig, et al Phys. Scr. (2011)

  4. Exposure with He strongly reduces D retention and permeation Molecular dynamics predicts hydrogen decoration of He bubbles (1 – 2 ML deep into matrix), clarifies growth mechanisms N. Juslin & B. D. Wirth, J. Nucl. Mater. (2013); F. Sefta, et al. Nucl. Fusion (2013). D2+He exposure reduces D retention to detection limit Mechanism: (1) He bubble network provides a pathway for H isotope release, or (2) He bubble induced stress acts to trap diffusing H isotopes R. Doerner et al, Nucl. Mater. Energy (2016); M. Baldwin et al, Nucl. Fusion (2011) W. R. Wampler et al, Nucl. Fusion (2009) Y. Uemura et al., presented at ICFRM-17.

  5. Many aspects of neutron damage can be investigated using high E ions • Retention too high for TBR > 1 in low fluence damaged tungsten; need damage study at higher fluencew/wo He 20x reduction 643 K data from PISCES-B 0.2 dpa 380 K 0.2 dpa 1200 K Projected 1000 K retention 0.3 dpa 320 K neutrons Upper limit On trapping probability 643 K data – PISCES-B 1 week FW fluence 10 weeks FW Fluence • Recent ion damage + simultaneous exposure of material to low energy D (Markelj et al, PSI 2016). • D may stabilize defects during exposure. G. Tynan, et al., PSI 2016.

  6. Data on retention / permeation of neutron damaged materials is limited • TITAN and PHENIX program providing first results • Retention at 500 °C increased dramatically by neutron irradiation M. Shimada, et al., Nucl. Fusion 2015.

  7. Potential Topics for Priority Research Directions Near Term Topics • Characterize the details of defects produced by ion / neutron irradiation to compare with simulations • Investigate observed reduction of retention / permeation due to concurrent D/He plasma exposure for ion and neutron damaged W • Measure temperature gradient effects on H diffusion (Soret effect: Q*) Longer Term Topics • Resolve discrepancies between H isotope retention in neutron and ion damaged W • Develop methods for the measurement of tritium retention / permeation needed at high temperatures and longer length scales • Investigate increased permeation in a radiation field (neutron / gamma) • Incorporate improved understanding of damage/diffusion/trapping into integrated PFC model

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